Demth137 Calculus
Demth137 Calculus
DEMTH137
Edited by
Dr. Kulwinder Singh
Calculus
Edited By:
Dr. Kulwinder Singh
CONTENT
Objectives
Students will be able to
Introduction
You have the idea about the number system since you began your journey of learning mathematics.
In this unit we will learn about some more properties of real numbers, the concept of sequence of real
numbers and their properties of being bounded and of convergence.
Absolute function
Let 𝑥 be a real number then there exist three possibilities, then it can be more than, less than or equal
to zero. The modulus value or absolute value of 𝑥 is defined as
𝑥 𝑖𝑓 𝑥 ≥ 0
|𝑥| = { ∀𝑥 ∈ℝ
−𝑥 𝑖𝑓 𝑥 < 0
Moreover, we can write |𝑥| = max {𝑥, −𝑥}.
Sequence is a kind of ordered list of numbers where a pattern can be seen. For example, 3, 6, 9, . . . is
a list in which the first term is 3, second is 6 and so on. We can easily tell that the fourth term will be
12 and so on. This example here is of an infinite sequence.
Technically, a function whose domain is a set of natural numbers and range is a subset of real
numbers, is called a real sequence (and just sequence in this course). Since the domain of all sequences
is the set of natural numbers, therefore a sequence is completely determined if
𝑓(𝑛) ∀ 𝑛 𝜖 𝑵 is known. The sequence 𝑓 is denoted as < 𝑓𝑛 > 𝑜𝑟 {𝑓𝑛 } mostly.
1
{ } , {(−1)𝑛 } etc.
𝑛
Range of sequence is the set of all distinct terms of a sequence. It can be infinite or finite. The first
sequence in the example is an infinite one and the second one is finite.
A sequence {𝑓𝑛 } is bounded above if there exists a real number K such that
𝑓𝑛 ≤ 𝐾 ∀ 𝑛𝜖𝑵
A sequence {𝑓𝑛 } is bounded below if there exists a real number k such that
𝑓𝑛 ≥ 𝑘 ∀ 𝑛𝜖𝑵
𝑘 ≤ 𝑓𝑛 ≤ 𝐾 ∀ 𝑛 𝜖 𝑵
Prove that the sequence {n} is not convergent and is not bounded.
1 1
Let 𝑝 be a real number. Then, the neighbourhood (𝑝 − , 𝑝 + ) will contain at most one term of the
4 4
sequence {𝑛}. Therefore, in this neighbourhood, we cannot find infinitely many terms of the sequence.
Hence the sequence is not convergent.
On the other hand, we can see that all the elements of the sequence are more than 1 but we cannot
find any upper bound i.e. any number so that all the elements of the sequence are below that number.
Therefore, the sequence is just bounded below and not bounded above or simply the sequence is not
bounded.
That is in any neighbourhood of 𝑎 , 𝑓𝑛 belongs to the same neighbourhood for infinite values of 𝑛.
Consider the sequence {𝑛}. If you consider any neighbourhood of any number 𝑎, it will not
contain an infinite number of elements of the sequence. On the other hand any neighbourhood of
1
any number a , for the sequence { } will contain infinitely many elements of the sequence.
𝑛
𝑙𝑖𝑚 𝑙𝑖𝑚
If 𝑛→∞ 𝑓𝑛 = 𝐴 and 𝑛→∞ 𝑔𝑛 = 𝐵, then
𝑙𝑖𝑚
(i) 𝑛→∞ ( 𝑓𝑛 + 𝑔𝑛 ) = 𝐴 + 𝐵
𝑙𝑖𝑚
(ii) 𝑛→∞ ( 𝑓𝑛 − 𝑔𝑛 ) = 𝐴 − 𝐵
(iii) 𝑙𝑖𝑚 𝑓𝑛 . 𝑔𝑛 = 𝐴. 𝐵
𝑛→∞
𝑙𝑖𝑚 𝑓 𝐴
(iv) 𝑛→∞ ( 𝑛) = provided 𝐵 ≠ 0
𝑔𝑛 𝐵
If B=0, A≠0 then the limit does not exist and if B=0, A=0 then the limit may or may not exist.
𝑙𝑖𝑚 𝑝
(v) 𝑛→∞ 𝑓𝑛 = 𝐴𝑝 , 𝑝𝜖𝑹
𝑆1 = 𝑓1
𝑆2 = 𝑓1 + 𝑓2
𝑆3 = 𝑓1 + 𝑓2 + 𝑓3
.
.
.
𝑆𝑛 = 𝑓1 + 𝑓2 + 𝑓3 + ⋯ + 𝑓𝑛
Here 𝑆𝑛 is called the 𝑛𝑡ℎ partial sum. The sequence 𝑆1 , 𝑆2 , 𝑆3 , . .. is symbolized by
𝑓1 + 𝑓2 + 𝑓3 + ⋯ = f
n =1
n
Can you recognize what kind of sequence is being depicted by the following graphs?
2𝑛−7
Prove that the sequence { } is (i) monotonically increasing (ii) is bounded and (iii)
3𝑛+2
2
tends to limit { }.
3
2𝑛−7
Let 𝑓𝑛 =
3𝑛+2
2𝑛−5
then 𝑓𝑛+1 =
3𝑛+5
2𝑛−5 2𝑛−7 25
And 𝑓𝑛+1 − 𝑓𝑛 = − = (3𝑛+5)(3𝑛+2) > 0 ∀ 𝑛 ∈ 𝑵
3𝑛+5 3𝑛+2
This shows that the given sequence is monotonically increasing. Now if we write few terms of the
sequence {𝑓𝑛 } , we can observe that all the terms are more than or equal to −1.
i.e. 𝑓𝑛 ≥ −1 ∀ 𝑛 ∈ 𝑵
𝑛+9
Moreover 1 − 𝑓𝑛 = > 0 ∀𝑛 ∈𝑵
3𝑛+2
7
2−
𝑙𝑖𝑚 𝑙𝑖𝑚 2𝑛−7 𝑙𝑖𝑚 𝑛 2
𝑛→∞ 𝑓𝑛 = 𝑛→∞ 3𝑛+2 = 𝑛→∞ 2 =3
3+
𝑛
Summary
In this chapter we have seen the concept of the sequence, its convergence, boundedness, and
monotonicity.
Key words
Real Numbers, Sequence, Series, Convergence, Bounded function, Monotonic function
Self Assessment
(a) 𝑥
(b) −𝑥
(c) min{−𝑥, 𝑥}
(d) max {−𝑥, 𝑥}
(a) [2,8]
(b) (2,8)
(c) (2,8]
(d) (-2,8)
True
False
True
False
𝑙𝑖𝑚 𝑙𝑖𝑚
11. If 𝑛→∞ 𝑓𝑛 = 𝐴 and 𝑛→∞ 𝑔𝑛 = 𝐵, then
(a) 𝑙𝑖𝑚 ( 𝑓𝑛 + 𝑔𝑛 ) = 𝐴 + 𝐵
𝑛→∞
(b) 𝑙𝑖𝑚 ( 𝑓𝑛 − 𝑔𝑛 ) = −𝐴 − 𝐵
𝑛→∞
(c) 𝑙𝑖𝑚 𝑓𝑛 . 𝑔𝑛 = 𝐴 + 𝐵
𝑛→∞
2𝑛−7
12. The sequence { } converges to
3𝑛+2
(a) 2/3
(b) -1
(c) 1
(d) none of these
(a) 𝑓𝑛+1 ≤ 𝑓𝑛 ∀ 𝑛 ∈ 𝑁
(b) 𝑓𝑛+1 < 𝑓𝑛 ∀ 𝑛 ∈ 𝑁
(c) 𝑓𝑛+1 > 𝑓𝑛 ∀ 𝑛 ∈ 𝑁
(d) 𝑓𝑛+1 ≥ 𝑓𝑛 ∀ 𝑛 ∈ 𝑁
(a) 𝑓𝑛+1 ≤ 𝑓𝑛 ∀ 𝑛 ∈ 𝑁
(b) 𝑓𝑛+1 < 𝑓𝑛 ∀ 𝑛 ∈ 𝑁
(c) 𝑓𝑛+1 > 𝑓𝑛 ∀ 𝑛 ∈ 𝑁
(d) 𝑓𝑛+1 ≥ 𝑓𝑛 ∀ 𝑛 ∈ 𝑁
(a) convergent
(b) monotonic
(c) convergent and monotonic
(d) neither convergent nor monotonic
Answers:
1 c 6 bounded 11 a
2 d 7 True 12 a
3 b 8 True 13 d
4 a 9 d 14 c
5 b 10 c 15 B
Review Questions
1. What is the solution of |𝑥 − 1| < 5 ?
2. Check whether the sequence {(−𝑛)𝑛 } is bounded or not?
3. What is the solution of |𝑥 − 2| < 6 ?
4. What is the solution of |𝑥 − 1| > 5 ?
5. Prove that |𝑎𝑏| = |𝑎||𝑏|.
6. State true or false: {𝑥: |𝑥 − 3| < 4} = {𝑥: −1 < 𝑥 < 7}
𝑙𝑖𝑚 𝑛
7. Evaluate 𝑛→∞ log 5
log9 (𝑛)
Further/Suggested Readings
1. George B. Thomas Jr., Joel Hass, Christopher Heil & Maurice D. Weir (2018). Thomas’
Calculus (14th edition). Pearson Education.
2. Howard Anton, I. Bivens & Stephan Davis (2016). Calculus (10th edition). Wiley India.
3. http://mathonline.wikidot.com/calculus
Notes
Objectives
Students will -
Introduction
You have learnt the rules of differentiation and integration at the senior secondary level. The definite
integral of a function gives you the area under the curve of that function between the specified limits.
In this unit we will look into the detail as to what is the integral as a limit of sum. We will evaluate
some definite integrals with this ab initio method. The functions can be classified as algebraic and
transcendental functions. The polynomial functions, rational functions are the algebraic functions
and exponential, logarithmic, trigonometric, inverse trigonometric functions, hyperbolic functions,
inverse hyperbolic functions are the examples of the transcendental functions. We will solve some
problems on integration of irrational as well as transcendental functions in this unit.
Notes First idea is to divide the interval [𝑎, 𝑏] onto 𝑛 equal sub-intervals as:
𝑏−𝑎
𝑎 = 𝑥0 , 𝑥1 , 𝑥2 , … , 𝑥𝑛−2 , 𝑥𝑛−1 , 𝑥𝑛 = 𝑏 . Now we can see that the length of each sub interval must be
𝑛
and let it be denoted by ℎ. Therefore we can write the points of the partition as follows:
𝑥0 = 𝑎,
𝑥1 = 𝑎 + ℎ
𝑥2 = 𝑎 + 2ℎ
.
.
.
𝑥𝑛 = 𝑎 + 𝑛ℎ = 𝑏
Clearly as → ∞ , ℎ → 0. In the above figure The region PRSQP is the sum of all the 𝑛 sub-regions,
where each sub-region is defined on sub-interval [𝑥𝑟−1 , 𝑥𝑟 ], 𝑟 = 1, 2, 3, … 𝑛. Observe region ABDM.
Area of the rectangle (ABLC) < Area of the region (ABDCA) < Area of the rectangle (ABDM).
As ℎ → 0 all these areas become almost equal to each other. Hence, we have
𝑛−1
and
𝑛
Here 𝑠𝑛 and 𝑆𝑛 denote the sum of areas of all lower rectangles and upper rectangles raised over
subintervals [𝑥𝑟−1 , 𝑥𝑟 ], 𝑟 = 1, 2, 3, … 𝑛 respectively.
Therefore we can write
𝑠𝑛 < area of the region < 𝑆𝑛
As 𝑛 → ∞, these strips become narrower. Further it is assumed that the limiting value of 𝑠𝑛 and 𝑆𝑛
are the same in both cases and the common limiting value is the required area under the curve.
Symbolically we can write
𝑏
𝑙𝑖𝑚 𝑠𝑛 = 𝑙𝑖𝑚 𝑆𝑛 =area (PRSQP) =∫𝑎 𝑓(𝑥)𝑑𝑥
𝑛→∞ 𝑛→∞
This area is also the limiting value of any area which is between that of the rectangles below the curve
and that of the rectangles above the curve. For convenience, we shall take the rectangles having
height equal to that of the curve at the left-hand-edge of each sub- interval. Hence, we can write
𝑏
∫ 𝑓(𝑥)𝑑𝑥 = 𝑙𝑖𝑚 ℎ[𝑓(𝑎) + 𝑓(𝑎 + ℎ) + ⋯ + 𝑓(𝑎 + (𝑛 − 1)ℎ)]
𝑎 𝑛→∞
5
Evaluate ∫2 𝑥 2 𝑑𝑥 as a limit of sum.
Here 𝑓(𝑥) = 𝑥 2
𝑏−𝑎 3
𝑎 = 2, 𝑏 = 5, ℎ = =
𝑛 𝑛
𝑏
Notes
∫ 𝑓(𝑥)𝑑𝑥 = 𝑙𝑖𝑚 ℎ[𝑓(𝑎 + ℎ) + 𝑓(𝑎 + 2ℎ) + ⋯ + 𝑓(𝑎 + 𝑛ℎ)]
𝑎 𝑛→∞
5
3
∫ 𝑥 2 𝑑𝑥 = 𝑙𝑖𝑚 [(2 + ℎ)2 + (2 + 2ℎ)2 + ⋯ + (2 + 𝑛ℎ)2 ]
2 𝑛→∞ 𝑛
3
= 𝑙𝑖𝑚 [𝑛 ⋅ 22 + ℎ2 (12 + 22 + ⋯ + 𝑛2 ) + 4ℎ(1 + 2 + ⋯ 𝑛)]
𝑛→∞ 𝑛
3 1 1 2 1
3 2
3 2 𝑛 (1 + 𝑛) (2 + 𝑛) 3 𝑛 (1 + 𝑛)
= 𝑙𝑖𝑚 [𝑛 ⋅ 2 + ( ) ( ) + 4( )( )]
𝑛→∞ 𝑛 𝑛 6 𝑛 2
1 1 1
(1 + ) (2 + ) (1 + )
= 𝑙𝑖𝑚 [3. 22 + 3(3)2 ( 𝑛 𝑛 ) + 3(4)(3) ( 𝑛 )]
𝑛→∞ 6 2
= 12 + 9 + 18 = 39
Thus the limit of the sum or in other words the area under the curve 𝑥 2 between lines 𝑥 = 2 and 𝑥 =
5 and above the 𝑥-axis is 39 square units.
𝑏
Evaluate ∫𝑎 cos 𝑥 𝑑𝑥 as the limit of a sum.
ℎ ℎ
2 sin ( ) 𝑆 = 2 sin ( ) ( cos(𝑎 + ℎ) + cos(𝑎 + 2ℎ) + cos(𝑎 + 3ℎ) + ⋯ + cos(𝑎 + 𝑛ℎ)
2 2
3 1 5 3 2𝑛+1
= sin (𝑎 + ℎ) − sin (𝑎 + ℎ) + sin (𝑎 + ℎ) − sin (𝑎 + ℎ) + … + sin (𝑎 + ℎ) −
2 2 2 2 2
2𝑛−1
sin (𝑎 + ℎ)
2
2𝑛+1 1
= sin (𝑎 + ℎ) − sin (𝑎 + ℎ)
2 2
1 1
= sin (𝑏 + ℎ) − sin (𝑎 + ℎ) as 𝑛ℎ = 𝑏 − 𝑎
2 2
1 1
𝑏 sin(𝑏+ ℎ)−sin(𝑎+ ℎ)
Thus ∫𝑎 cos 𝑥 𝑑𝑥 = 𝑙𝑖𝑚 ℎ 2
ℎ
2
𝑛→∞ 2 sin( )
2
= sin 𝑏 − sin 𝑎
In the senior secondary level, you have learnt how to integrate the algebraic rational functions and
the trigonometric functions. In the next section we will see some cases of the integration of irrational
algebraic function.
𝑏 1
Evaluate ∫𝑎 𝑑𝑥 as limit of sum.
√𝑥
Notes
2.2 Integration of irrational algebraic functions
Certain types of integrals containing irrational expressions can be reduced to integrals of rational
functions by making appropriate substitutions. These substitutions are done with an intention to
convert the irrational function into a rational one.
𝑚
To integrate a function that contains only one irrational expression of the form 𝑥 𝑛 we
1
make the substitution for 𝑥 𝑛 .
1 1
𝑎𝑥+𝑏 𝑛 𝑎𝑥+𝑏 𝑛
An expression of the form ( ) can be integrated by using the substitution for ( ) , where
𝑐𝑥+𝑑 𝑐𝑥+𝑑
𝑎, 𝑏, 𝑐, 𝑑 are real numbers. These substitutions reduce the integrals rational functions in the
transformed variable.
The integrals containing radicals of the form √𝑎2 − 𝑥 2 , √𝑎2 + 𝑥 2 and √𝑥 2 − 𝑎2 can be evaluated with
the help of trigonometric and hyperbolic substitutions.
𝑥
Consider the integral of ∫ 1 𝑑𝑥
(𝑎+𝑏𝑥)3
The denominator is having an irrational function and if we substitute 𝑎 + 𝑏𝑥 = 𝑦 3 then the given
integrand can be written as a rational function in 𝑦. Let us see the steps.
If we substitute 𝑎 + 𝑏𝑥 = 𝑦 3
Then 𝑏 𝑑𝑥 = 3𝑦 2 𝑑𝑦
𝑥 𝑦 3 −𝑎 3𝑦 2
And ∫ 1 𝑑𝑥 = ∫ ( )( ) 𝑑𝑦
(𝑎+𝑏𝑥)3 𝑏 𝑦𝑏
1
= ∫ (𝑦 4 − 𝑎𝑦)𝑑𝑦
𝑏2
3 𝑦5 𝑎𝑦 2
= [ − ]+C
𝑏2 5 2
3
= 𝑦 2 (2𝑦 3 − 5𝑎) + 𝐶
10𝑏2
√𝑥+9
Evaluate ∫ ( ) 𝑑𝑥
𝑥
Put √𝑥 + 9 = 𝑢
𝑑𝑥 = 2 𝑢 𝑑𝑢
Then
√𝑥+9 𝑢 𝑢2
∫( ) 𝑑𝑥 = ∫ ( ) 2𝑢𝑑𝑢 = 2 ∫ 𝑑𝑢
𝑥 𝑢2 −9 𝑢2 −9
𝑢2 −9+9
= 2∫ 𝑑𝑢-
𝑢2 −9
9
= 2 ∫ 𝑑𝑢 + 2∫ 𝑑𝑢
𝑢2 − 9
1 𝑢−3
= 2 𝑢 + 2. 9. ln | |+𝐶
6 𝑢+3
= 2 √𝑥 + 9 + 3 ln |(√𝑥 + 9 − 3)/(√𝑥 + 9 + 3) + 𝐶
where 𝐶 is the constant of integration.
1
Evaluate ∫ (5𝑥 − 1)3 𝑑𝑥
1
To solve this integral, substitute (5𝑥 − 1)3 = 𝑢
Notes
(5𝑥 − 1) = 𝑢3
5 𝑑𝑥 = 3 𝑢2 𝑑𝑢
Then
1 3𝑢2
∫ (5𝑥 − 1)3 𝑑𝑥 = ∫ 𝑢 𝑑𝑢
5
3 4
= 𝑢 +𝐶
20
3 4
= (5𝑥 − 1)3 + 𝐶
20
2.3 Integration of transcendental functions
A number that is not the root of any integer polynomial is termed as a transcendental number. And
on the same lines a function that cannot be written using roots and the arithmetic found in
polynomials is known as a transcendental function.
e.g. Exponential function
Logarithmic function
Trigonometric function
Inverse trigonometric function
Hyperbolic function
Inverse hyperbolic functions etc.
You are familiar with all the above mentioned functions except the hyperbolic
function. So here is a short introduction to this family of transcendental functions.
Hyperbolic functions are the functions defined in terms of the exponential functions as follows.
Just like with trigonometric functions, there are identities related to the hyperbolic functions.
Rules of differentiation and integration are as follows. Here the prime symbol is for denoting the first
derivative.
Notes
The graphs of the hyperbolic functions are shown below and it can be seen that with appropriate
range restrictions, they all have inverses (same as the case with the inverse trigonometric functions).
Notes
The range in case of sec ℎ−1 𝑥 is [0, ∞) and for coth−1 𝑥 is (−∞, 0)𝑈(0, ∞). The derivative of the
inverse hyperbolic functions are as follows:
The integral as an anti-derivative can be written easily from the above rules of differentiation.
Notes Thus you got a brief idea about the calculus of hyperbolic functions and inverse hyperbolic functions.
For more information you can check the following link.
https://math.libretexts.org/Courses/Monroe_Community_College/MTH_21
1_Calculus_II/Chapter_6%3A_Applications_of_Integration/6.9%3A_Calculus
_of_the_Hyperbolic_Functions
Now with the knowledge of the transcendental functions, we can look into the examples related to
the integration of the transcendental functions.
𝑥𝑒 𝑥
Evaluate ∫ (𝑥+1)2
𝑑𝑥
𝑥𝑒 𝑥 (𝑥 + 1 − 1)𝑒 𝑥
∫ 𝑑𝑥 = ∫ 𝑑𝑥
(𝑥 + 1)2 (𝑥 + 1)2
1 1
=∫ ( − (𝑥+1)2) 𝑒 𝑥 𝑑𝑥
𝑥+1
𝑒𝑥
= +𝐶 (Using integration by parts on the first term)
𝑥+1
Put log 𝑥 = 𝑡
1
i.e. 𝑑𝑥 = 𝑑𝑡
𝑥
𝑑𝑥 = 𝑒 𝑡 𝑑𝑡
Therefore ∫ sin (log 𝑥) 𝑑𝑥 = ∫ 𝑒 𝑡 sin𝑡 𝑑𝑡
= −𝑒 −𝑡 cos 𝑡 + 𝑒 𝑡 sin 𝑡 − ∫ 𝑒 𝑡 sin𝑡 𝑑𝑡
Clubbing the integral term, we get
2∫ 𝑒 𝑡 sin 𝑡 𝑑𝑡 = 𝑒 𝑡 (sin 𝑡 − cos 𝑡) + 𝐶
𝑒𝑡 𝐶
∫ 𝑒 𝑡 sin 𝑡 𝑑𝑡 = (sin 𝑡 − cos 𝑡) +
2 2
1
∫ sin (log 𝑥) 𝑑𝑥 = 𝑥(sin (log 𝑥) − cos (𝑙𝑜𝑔𝑥)) + 𝑪
2
𝑒 𝑎𝑥 𝑏 𝑎𝑥
𝐼= cos (𝑏𝑥 + 𝑐) + ∫ ( ) sin (𝑏𝑥 + 𝑐) 𝑒 𝑑𝑥
𝑎 𝑎
𝑒 𝑎𝑥 𝑏 𝑎𝑥 𝑏2 𝑎𝑥
𝐼= cos (𝑏𝑥 + 𝑐) + (𝑎2) sin (𝑏𝑥 + 𝑐) 𝑒 − 𝑎2 ∫ 𝑐𝑜𝑠(𝑏𝑥 + 𝑐) 𝑒 𝑑𝑥 (integrating by parts)
𝑎
𝑏2 𝑒 𝑎𝑥
(1 + ) 𝐼 = (𝑎 cos(𝑏𝑥 + 𝑐) + 𝑏 sin (𝑏𝑥 + 𝑐))
𝑎2 𝑎2
𝑒 𝑎𝑥
𝐼= ( 𝑎 cos(𝑏𝑥 + 𝑐) + 𝑏 sin(𝑏𝑥 + 𝑐))
𝑎2 + 𝑏2
1−𝑥
Integrate tan−1 √ with respect to 𝑥.
1+𝑥
1−𝑥
Let 𝐼 = tan−1 √
1+𝑥
Notes
Put 𝑥 = cos 𝜃
𝑑𝑥 = − sin 𝜃 𝑑𝜃
1
= − (−𝜃 cos 𝜃 + 𝑠𝑖𝑛𝜃)
2
1
= − (−𝑥 cos −1 𝑥 + √1 − 𝑥 2 ) + 𝐶
2
𝑠𝑖𝑛ℎ𝑥
Evaluate ∫ 𝑑𝑥
1+𝑐𝑜𝑠ℎ𝑥
Put sin 𝑥 = 𝑢
cos 𝑥 𝑑𝑥 = 𝑑𝑢
1
𝐼=∫ 𝑑𝑢 (Refer to the rules of differentiation (integration) of the inverse hyperbolic functions)
√1+𝑢2
= sinh−1 𝑢 + 𝐶
= sinh−1 sin 𝑥 + 𝐶
1
Evaluate the integral ∫ 𝑑𝑥
√4𝑥 2 −1
Let us substitute 2𝑥 = 𝑢
2𝑑𝑥 = 𝑑𝑢 and this results in
1 1
∫ 𝑑𝑥 = ∫ 𝑑𝑢
√4𝑥 2 −1 2√𝑢2 − 1
1
= cosh−1 𝑢 + 𝐶
2
1
= cosh−1 (2𝑥) + 𝐶
2
Summary
In this chapter we have seen how a definite integral can be calculated as a limit of sum. This is the ab
initio way to calculate the area under a curve 𝑦 = 𝑓(𝑥) bounded by the two vertical lines 𝑥 = 𝑎, 𝑥 =
𝑏 and the x-axis.
Key words
Real Numbers, Sequence, Series, Convergence, Bounded function, Monotonic function
Notes
Review Questions
Evaluate the following:
1. ∫ sinh3 𝑥 cosh 𝑥 𝑑𝑥
2. ∫ sech2 3𝑥 𝑑𝑥
𝑑
3. (cosh−1 3𝑥)
𝑑𝑥
1
4. ∫ √1−𝑒 2𝑥 𝑑𝑥
5. ∫ √𝑒 𝑥 + 1𝑑𝑥
𝑥 2 −2
6. ∫ 𝑑𝑥
𝑥+1
1−𝑥 𝑑𝑥
7. ∫
1+𝑥 𝑥
8. ∫ √𝑠𝑒𝑐𝑥 − 1 𝑑𝑥
𝑑𝑥
9. ∫
5+4𝑐𝑜𝑠𝑥
10. ∫ 𝑐𝑜𝑠𝑒𝑐 5 𝑥 𝑑𝑥
11. ∫ sinh3 𝑥 𝑑𝑥
12. ∫ 𝑥 sinh 𝑥 𝑑𝑥
3
13. Evaluate the definite integral ∫2 𝑥 3 𝑑𝑥 as limit of sum.
𝑏
14. Evaluate the definite integral ∫𝑎 sinh 𝑥 𝑑𝑥 as limit of sum.
𝜋/2
15. Evaluate the definite integral ∫0 cos 𝑥 𝑑𝑥 as limit of sum.
Further/Suggested Readings
George B. Thomas Jr., Joel Hass, Christopher Heil & Maurice D. Weir (2018). Thomas’ Calculus
(14th edition). Pearson Education.
Howard Anton, I. Bivens & Stephan Davis (2016). Calculus (10th edition). Wiley India.
Shanti Narayan & Dr. P. K. Mittal (2018). Integral Calculus (11th edition). S. Chand
Objectives
Students will
Introduction
By now, you are well aware of the methods of substitution, method of integration by parts and the
method in which we decompose the given integrand in the sum of integrands with known integrals.
There is one more technique and that is called integration by successive reduction or integration
using reduction formula.
Here the integrand is 𝑥 𝑛 𝑒 𝑎𝑥 . This is a general form of the function. In the reduction formula we seek
a relation of the given integral with another integral having the same form but involving 𝑛 − 1 or 𝑛 −
2 etc. And that can be accomplished by integrating the given integral by parts.
Let 𝐼𝑛 = ∫ 𝑥 𝑛 𝑒 𝑎𝑥 𝑑𝑥
Integrating by parts, we get
𝑥 𝑛 𝑒 𝑎𝑥 𝑥 𝑛−1 𝑒 𝑎𝑥
𝐼𝑛 = −∫𝑛 𝑑𝑥
𝑎 𝑎
𝑥 𝑛 𝑒 𝑎𝑥 𝑛
𝐼𝑛 = − 𝐼𝑛−1
𝑎 𝑎
Here you can see that 𝐼𝑛−1 is having the same type as that of given integral except that the ′𝑛′ has
reduced to ′𝑛 − 1′ . Hence you can see the justification for the name ‘reduction formula’ also.
Now if we need to calculate ∫ 𝑥 3 𝑒 𝑎𝑥 𝑑𝑥, we know what to do!
𝑥 𝑛 𝑒 𝑎𝑥 𝑛
In the reduction formula 𝐼𝑛 = − 𝐼𝑛−1 we will get 𝐼3 in terms of 𝐼2 , 𝐼2 in terms of 𝐼1 and 𝐼1 in
𝑎 𝑎
terms of 𝐼0 . The last integral in the recursion 𝐼0 is so easy to calculate. Then backward substitution
leads to the required integral.
Let’s see how it goes.
𝑥 3 𝑒 𝑎𝑥 3
𝐼3 = − 𝐼2 -----(1)
𝑎 𝑎
𝑥 2 𝑒 𝑎𝑥 2
𝐼2 = − 𝐼1 -----(2)
𝑎 𝑎
𝑥 1 𝑒 𝑎𝑥 1
𝐼1 = − 𝐼0 -----(3)
𝑎 𝑎
𝑥 3 𝑒 𝑎𝑥 3 𝑥 2 𝑒 𝑎𝑥 2 𝑥1 𝑒 𝑎𝑥 1 𝑒 𝑎𝑥
𝐼3 = − ( − ( − ))
𝑎 𝑎 𝑎 𝑎 𝑎 𝑎 𝑎
𝑥 3 𝑒 𝑎𝑥 3𝑥 2 𝑒 𝑎𝑥 6𝑥𝑒 𝑎𝑥 𝑒 𝑎𝑥
= − 2
+ 3
−6 4
𝑎 𝑎 𝑎 𝑎
which is the required solution.
In this integral, there are two parameters 𝑚 and 𝑛. In order to have a reduction formula, let us
integrate by parts taking 𝑥 𝑚 as the first function and sin 𝑛𝑥 as the second function.
𝑥 𝑚 𝑐𝑜𝑠𝑛𝑥 𝑚
∫ 𝑥 𝑚 sin𝑛𝑥 𝑑𝑥 = − + ∫ 𝑥 𝑚−1 cos 𝑛𝑥𝑑𝑥
𝑛 𝑛
Again integrating by parts,
𝑥 𝑚 𝑐𝑜𝑠𝑛𝑥 𝑚𝑥 𝑚−1 𝑠𝑖𝑛𝑛𝑥 𝑚(𝑚 − 1)
∫ 𝑥 𝑚 sin𝑛𝑥 𝑑𝑥 = − + − ∫ 𝑥 𝑚−2 sin 𝑛𝑥𝑑𝑥
𝑛 𝑛2 𝑛2
Therefore here we got the relation in two integrals of the same type but the one on the right side is of
lower degree. The left side integral can be written as 𝐼𝑚,𝑛 and the right-side integral which is reduced
version can be written as 𝐼𝑚−2,𝑛 .
∞
Establish a reduction formula for ∫ 𝑥 𝑛 𝑒 −𝑥 𝑑𝑥 and deduce that ∫0 𝑥 𝑛 𝑒 −𝑥 𝑑𝑥 = 𝑛! where 𝑛 is
any natural number.
∫ 𝑥 𝑛 𝑒 −𝑥 𝑑𝑥 = −𝑥 𝑛 𝑒 −𝑥 + 𝑛∫ 𝑥 𝑛−1 𝑒 −𝑥 𝑑𝑥
Or
𝐼𝑛 = −𝑥 𝑛 𝑒 −𝑥 + 𝑛𝐼𝑛−1 is the required reduction formula. Now for the deduction, consider the
integral,
𝑡 𝑡
∫ 𝑥 𝑛 𝑒 −𝑥 𝑑𝑥 = |−𝑥 𝑛 𝑒 −𝑥 |𝑡0 + 𝑛 ∫ 𝑥 𝑛−1 𝑒 −𝑥 𝑑𝑥
0 0
𝑡
= −𝑡 𝑛 𝑒 −𝑡 + 𝑛 ∫ 𝑥 𝑛−1 𝑒 −𝑥 𝑑𝑥
0
Or 𝐼𝑛 = 𝑛𝐼𝑛−1
𝐼𝑛−1 = (𝑛 − 1)𝐼𝑛−2
𝐼𝑛−2 = (𝑛 − 2)𝐼𝑛−3
𝐼𝑛−3 = (𝑛 − 3)𝐼𝑛−4
.
.
.
𝐼1 = 1. 𝐼0 = 1 (The integral 𝐼0 can easily be calculated to be 1.)
By back substitution we get
𝐼𝑛 = 𝑛(𝑛 − 1)(𝑛 − 2) … 3.2.1 = 𝑛!
𝑥𝑛
Establish the reduction formula for ∫ (𝑙𝑜𝑔𝑥)𝑚
𝑑𝑥
In this integral, there are two parameters, and the idea is to get a relation of the given integral with
another integral of same type but reduced parameter(s) any one or both.
To integrate the given function, let us write the integrand in the following way:
1 1
𝐼𝑚,𝑛 = ∫ 𝑥 𝑛+1 [ . ] 𝑑𝑥
(𝑙𝑜𝑔𝑥)𝑚 𝑥
Now the integration by parts can be applied taking the term in bracket as the second function.
Therefore,
(log 𝑥)−𝑚+1 (log 𝑥)−𝑚+1
𝐼𝑚,𝑛 = 𝑥 𝑛+1 − ∫ (𝑛 + 1)𝑥 𝑛 𝑑𝑥
−𝑚 + 1 −𝑚 + 1
(log 𝑥)−𝑚+1 𝑛 + 1 𝑥𝑛
𝐼𝑚,𝑛 = 𝑥 𝑛+1 + ∫ 𝑑𝑥
−𝑚 + 1 𝑚−1 (log 𝑥)𝑚−1
(log 𝑥)−𝑚+1 𝑛+1
Or 𝐼𝑚,𝑛 = 𝑥 𝑛+1 + 𝐼 is the required reduction formula.
−𝑚+1 𝑚−1 𝑚−1,𝑛
𝜋
Evaluate ∫02 sin𝑛 𝑥 𝑑𝑥 where 𝑛 is a positive integer.
𝑥𝑛
Construct the reduction formula for ∫ 𝑑𝑥 where 𝑛 ∈ 𝑵
√𝑎𝑥 2 +𝑏𝑥+𝑐
Here the integrand is an irrational function and it can be re written by involving the derivative of the
term in the denominator as follows:
2𝑎𝑥 + 𝑏 − 𝑏 𝑛−1
𝑥𝑛 = 𝑥
2𝑎
1 (2𝑎𝑥 + 𝑏)𝑥 𝑛−1 𝑏 𝑥 𝑛−1
𝐼𝑛 = ∫ 𝑑𝑥 − ∫ 𝑑𝑥
2𝑎 √𝑎𝑥 2 + 𝑏𝑥 + 𝑐 2𝑎 √𝑎𝑥 2 + 𝑏𝑥 + 𝑐
1 𝑛−1 𝑏(𝑛 − 1) 𝑐(𝑛 − 1) 𝑏
𝐼𝑛 = 𝑥 √𝑎𝑥 2 + 𝑏𝑥 + 𝑐 − (𝑛 − 1) 𝐼𝑛 − 𝐼𝑛−1 − 𝐼𝑛−2 − 𝐼
𝑎 𝑎 𝑎 2𝑎 𝑛−1
1 𝑏(2𝑛−1) 𝑐(𝑛−1)
𝐼𝑛 = 𝑥 𝑛−1 √𝑎𝑥 2 + 𝑏𝑥 + 𝑐 − 𝐼𝑛−1 − 𝐼𝑛−2 is the required reduction formula.
𝑛𝑎 2𝑛𝑎 𝑛𝑎
𝑥3
Let us evaluate ∫ 𝑑𝑥. You can see that this integral is a particular case of the integral whose
√𝑥 2 −2𝑥+2
reduction formula is
𝑥𝑛 1 𝑏(2𝑛−1) 𝑥 𝑛−1 𝑐(𝑛−1) 𝑥 𝑛−2
∫ 𝑑𝑥 = 𝑥 𝑛−1 √𝑎𝑥 2 + 𝑏𝑥 + 𝑐 − ∫ 𝑑𝑥 − ∫ 𝑑𝑥
√𝑎𝑥 2 +𝑏𝑥+𝑐 𝑛𝑎 2𝑛𝑎 √𝑎𝑥 2 +𝑏𝑥+𝑐 𝑛𝑎 √𝑎𝑥 2 +𝑏𝑥+𝑐
𝑥2 1 3 𝑥1 1
Also ∫ 𝑑𝑥 = √𝑥 2 − 2𝑥 + 2 + ∫ 𝑑𝑥 − ∫ 𝑑𝑥 -----(2)
√𝑥 2 −2𝑥+2 2 2 √𝑥 2 −2𝑥+2 √𝑥 2 −2𝑥+2
Let us work on the two integrals on the right hand side of the equation (2).
𝑥 1 2𝑥 −2 1 2
∫ 𝑑𝑥 = ∫ 𝑑𝑥 + ∫ 𝑑𝑥 = (𝑥 2 − 2𝑥 + 2)1/2 + sinh−1 (𝑥 − 1) -----(3)
√𝑥 2 −2𝑥+2 2 √𝑥 2 −2𝑥+2 2 √(𝑥−1)2 +1
1
∫ 𝑑𝑥 = sinh−1 (𝑥 − 1) -----(4)
√𝑥 2 −2𝑥+2
𝑠𝑖𝑛𝑛𝑥
Form a reduction formula for ∫ 𝑑𝑥
𝑠𝑖𝑛𝑥
The parameter 𝑛 can be seen in the numerator of the integrand. Here integration by parts may not
help in getting a reduced form of the same type of integral. So we can use trigonometric identity
𝐶+𝐷 𝐶−𝐷
(sin 𝐶 − sin 𝐷 = 2 cos sin ) as follows:
2 2
Definite Integral
𝑏
The definite integral is an integral of the form ∫𝑎 𝑓(𝑥) 𝑑𝑥. This integral is read as the integral from a
to b of 𝑓(𝑥) 𝑑𝑥. The numbers a and b are said to be the limits of integration. For our problems, a is less
than b. Definite Integrals are evaluated using the Fundamental Theorem of Calculus.
For 𝐹 = 𝑓(𝑔(𝑥)) and 𝑢 = 𝑔(𝑥) we can use these ideas to rewrite the chain rule as follows:
𝑑𝐹 𝑑 𝑑𝑢 𝑑𝐹 𝑑𝑢
𝐹 ′ (𝑥) = = (𝑓(𝑔(𝑥)) = 𝑓 ′ (𝑔(𝑥))𝑔′ (𝑥) = 𝑓 ′ (𝑢) =
𝑑𝑥 𝑑𝑥 𝑑𝑥 𝑑𝑢 𝑑𝑥
This gives another way to write the chain rule, which is as follows:
This way of expressing the chain rule can be useful when using the Second Fundamental Theorem of
𝑔(𝑥) 𝑢
Calculus. Suppose 𝐹(𝑥) = ∫𝑎 𝑓(𝑡) 𝑑𝑡 , then taking 𝑢 = 𝑔(𝑥) gives 𝐹 = ∫𝑎 𝑓(𝑡) 𝑑𝑡
𝑑𝐹 𝑑𝑢 𝑑 𝑢 𝑑𝑢 𝑑𝑢
Then 𝐹 ′ (𝑥) = ⋅ = (∫𝑎 𝑓(𝑡) 𝑑𝑡 ) ⋅ = 𝑓(𝑢) ⋅ = 𝑓(𝑔(𝑥)) ⋅ 𝑔′ (𝑥)
𝑑𝑢 𝑑𝑥 𝑑𝑢 𝑑𝑥 𝑑𝑥
Properties
𝑏 𝑏
1. ∫𝑎 𝜙(𝑥)𝑑𝑥 = ∫𝑎 𝜙(𝑡)𝑑𝑡
Let ∫ 𝜙(𝑥)𝑑𝑥 = 𝐹(𝑥) + 𝑐1
and ∫ 𝜙(𝑡)𝑑𝑡 = 𝐹(𝑡) + 𝑐2
𝑏
Therefore, ∫𝑎 𝜙(𝑥)𝑑𝑥 = [𝐹(𝑥) + 𝑐1 ]𝑏𝑎 = 𝐹(𝑏) − 𝐹(𝑎)
𝑏
Similarly, ∫𝑎 𝜙(𝑡)𝑑𝑡 = 𝐹(𝑏) − 𝐹(𝑎)
This property explains the dummy nature of the variable of integration in a definite integral.
𝑏 𝑐 𝑏
2. ∫𝑎 𝜙(𝑥)𝑑𝑥 = ∫𝑎 𝜙(𝑥)𝑑𝑥 + ∫𝑐 𝜙(𝑥)
Let ∫ 𝜙(𝑥)𝑑𝑥 = 𝐹(𝑥) + 𝑐1
Then the RHS= [𝐹(𝑥) + 𝑐1 ]𝑐𝑎 + [𝐹(𝑥) + 𝑐1 ]𝑏𝑐
= 𝐹(𝑐) − 𝐹(𝑎) + 𝐹(𝑏) − 𝐹(𝑐)
= 𝐹(𝑏) − 𝐹(𝑎)
𝑏
= ∫ 𝜙(𝑥)𝑑𝑥 = 𝐿𝐻𝑆
𝑎
𝑏 𝑎
3. ∫𝑎 𝜙(𝑥)𝑑𝑥 = − ∫𝑏 𝜙(𝑥)𝑑𝑥
Let ∫ 𝜙(𝑥)𝑑𝑥 = 𝐹(𝑥) + 𝑐1
𝑎
Consider the RHS = − ∫𝑏 𝜙(𝑥)𝑑𝑥
= −[𝐹(𝑥) + 𝑐1 ]𝑎𝑏
= [𝐹(𝑎) + 𝑐1 − 𝐹(𝑏) − 𝑐1
𝑏
= 𝐹(𝑏) − 𝐹(𝑎) = ∫ 𝜙(𝑥)𝑑𝑥 = 𝐿𝐻𝑆
𝑎
𝑎 𝑎
4. ∫0 𝜙(𝑥)𝑑𝑥 = ∫0 𝜙(𝑎 − 𝑥)𝑑𝑥
Letting 𝑎 − 𝑥 = 𝑡
or 𝑥 = 𝑎 − 𝑡
or 𝑑𝑥 = −𝑑𝑡
𝑎 0 𝑎 𝑎
Now the RHS= ∫0 𝜙(𝑎 − 𝑥)𝑑𝑥 = − ∫𝑎 𝜙(𝑡)𝑑𝑡 = ∫0 𝜙(𝑡)𝑑𝑡 = ∫0 𝜙(𝑥)𝑑𝑥
𝑎
2𝑎 2 ∫0 𝜙(𝑥)𝑑𝑥 if 𝜙(2𝑎 − 𝑥) = 𝜙(𝑥)
5. ∫0 𝜙(𝑥)𝑑𝑥 = {
0 if 𝜙(2𝑎 − 𝑥) = −𝜙(𝑥)
2𝑎
Consider ∫𝑎 𝜙(𝑥)𝑑𝑥
𝑎 0 if 𝜙(−𝑥) = −𝜙(𝑥)
6. ∫−𝑎 𝜙(𝑥)𝑑𝑥 = { 𝑎
2 ∫0 𝜙(𝑥)𝑑𝑥 if 𝜙(−𝑥) = 𝜙(𝑥)
0
Consider ∫−𝑎 𝜙(𝑥)𝑑𝑥
𝜋/2
Evaluate ∫0 log(1 + 𝑡𝑎𝑛𝜃) 𝑑𝜃
𝜋
Let 𝐼 = ∫04 log(1 + 𝑡𝑎𝑛𝜃) 𝑑𝜃
𝜋
𝜋
= ∫04 log (1 + tan ( − 𝜃)) 𝑑𝜃
4
𝜋
4 1 − 𝑡𝑎𝑛𝜃
= ∫ log (1 + ) 𝑑𝜃
0 1 + 𝑡𝑎𝑛𝜃
𝜋
4 2
= ∫ log ( ) 𝑑𝜃
0 1 + 𝑡𝑎𝑛𝜃
𝜋
𝜋 4
= log 2 − ∫ log(1 + 𝑡𝑎𝑛𝜃) 𝑑𝜃
4 0
𝜋
Or 𝐼 = log 2
8
𝜋
Evaluate ∫0 𝑥 sin6 𝑥 cos4 𝑥 𝑑𝑥
𝜋
Let 𝐼 = ∫0 𝑥 sin6 𝑥 cos4 𝑥 𝑑𝑥
𝜋
= ∫ (𝜋 − 𝑥) sin6 (𝜋 − 𝑥) cos4 (𝜋 − 𝑥)𝑑𝑥
0
𝜋 𝜋
= ∫ (𝜋) sin6 (𝑥) cos4 (𝑥)𝑑𝑥 − ∫ (𝑥) sin6 (𝑥) cos4 (𝑥)𝑑𝑥
0 0
𝜋/2
2𝐼 = 2𝜋 ∫ sin6 𝑥 cos4 𝑥 𝑑𝑥
0
2𝜋 5.3.1.3.1 𝜋
𝐼=
2 10.8.6.4.2 2
3𝜋 2
𝐼=
512
Summary
In this chapter we have seen one more technique of solving the integral by writing a recursion
formula. Many general integrals can be solved by this method including their particular cases. We
have also seen the proofs of the properties of the definite integral.
Key words
Definite integral, reduction formula, properties of definite integral
Self-Assessment
3
1. ∫2 𝑥 3 𝑑𝑥 is equal to
(a) 65 (b) 65/4 (c) ¼ (d) 63/4
𝜋
2. If 𝑚 ≠ 𝑛, then ∫0 cos 𝑚𝑥 cos 𝑛𝑥 𝑑𝑥 is
𝜋
(a) 0 (b) (c) 𝜋 (d) 2𝜋
2
𝜋
3. ∫02 sin5 𝑥 𝑑𝑥 is
(a) 5/15 (b) 6/15 (c) 7/15 (d) 8/15
𝜋
4. ∫02 sin6 𝑥 𝑑𝑥 is
(a) 5/32 (b) 5𝜋/32 (c) 5/16 (d) 5𝜋/16
𝜋
5. ∫02 cos7 𝑥 𝑑𝑥 is
(a) 16/35 (b) 6/15 (c) 17/15 (d) 8/35
𝜋
6. ∫02 cos8 𝑥 𝑑𝑥 is
(a) 5/32 (b) 35𝜋/256 (c) 35/256 (d) 5𝜋/16
𝜋
7. ∫04 cos6 2𝑥 𝑑𝑥 is
(a) 5/64 (b) 5𝜋/64 (c) 35/256 (d) 𝜋/16
3
1
8. ∫0 𝑥 2 (1 − 𝑥 2 )2 𝑑𝑥 is
𝜋 𝜋 𝜋 𝜋
(a) (b) (c) (d)
32 16 8 4
𝜋/2 √𝑠𝑖𝑛𝑥
9. ∫0 𝑑𝑥 is
√𝑠𝑖𝑛𝑥+√𝑐𝑜𝑠𝑥
𝜋 𝜋 𝜋
(a) (b) (c) (d) None of these
2 4 8
𝜋
10. ∫0 𝑥𝑠𝑖𝑛6 𝑥𝑐𝑜𝑠 4 𝑥 𝑑𝑥 is
3𝜋2 3𝜋2 𝜋2
(a) 3𝜋 2 (b) (c) (d)
51 512 512
𝜋
11. ∫02 log sin 𝑥 𝑑𝑥 is
𝜋 𝜋 3𝜋 𝜋
(a) − log 2 (b) log 2 (c) − log 2 (d) −
2 2 2 2
𝜋
12. ∫0 log (1 + cos 𝑥)𝑑𝑥 is
(a) −𝜋 log 2 (b) 𝜋 log 1/2 (c) Both (a) and (b) (d) None of these
𝜋/2
13. ∫0 sin5 𝑥 cos6 𝑥 𝑑𝑥 is
(a) 8/693 (b) 8/69 (c) 8/6 (d) None of these
𝜋/2
14. ∫0 sin6 𝑥 cos8 𝑥 𝑑𝑥 is
5 5𝜋 𝜋
(a) (b) (c) (d) None of these
4096 4096 4096
𝜋/2
15. ∫0 cos 2𝑥 cos3 𝑥 𝑑𝑥 is
8 2 2 5
(a) (b) (c) (d)
15 15 5 2
Answers:
1 b 2 a 3 d 4 b 5 a
6 b 7 b 8 a 9 b 10 c
11 a 12 c 13 a 14 b 15 c
Review Questions
1. Construct the reduction formula for ∫ sin𝑝 𝑥 cos𝑞 𝑥 𝑑𝑥 where 𝑝, 𝑞 are positive integers.
𝜋/2
2. Evaluate the definite integral ∫0 sin𝑝 𝑥 cos𝑞 𝑥 𝑑𝑥 where 𝑝, 𝑞 are positive integers.
𝜋
3. Using the properties prove that ∫0 (𝑥 sin 𝑥)/(1 + cos2 𝑥) 𝑑𝑥 = 𝜋 2 /4.
𝜋/2 1
4. Using the properties prove that ∫0 sin2 𝑥/(sin 𝑥 + 𝑐𝑜𝑠 𝑥) 𝑑𝑥 = log(√2 + 1)
√2
𝜋/2
5. Evaluate ∫0 𝑥 cot 𝑥 𝑑𝑥 using the properties of definite integral.
Further/Suggested Readings
George B. Thomas Jr., Joel Hass, Christopher Heil & Maurice D. Weir (2018).
Thomas’ Calculus (14th edition). Pearson Education.
Howard Anton, I. Bivens & Stephan Davis (2016). Calculus (10th edition).
Wiley India.
https://www.intmath.com/integration/4-definite-integral.php
https://www.math24.net/properties-definite-integrals
https://www.intmath.com/methods-integration/10-integration-reduction-
formulae.php
Notes
Objectives
Students will
Introduction
In this unit we will understand one of the most crucial and fundamental concept of calculus. But
before that let us have an idea about the function. You can consider a function as a kind of rule
where you give in some input and get a specific output. The input is decided as everything that
keeps the function well defined. The technical name for such input is the domain. Let us see what a
function is! First of all there must be two non-empty sets 𝐴 and 𝐵, then a function 𝑓 from 𝐴 to 𝐵 is
denoted as 𝑓: 𝐴 → 𝐵 and is defined as a function if for all the values in set 𝐴, there corresponds a
unique value in set B. Set A is called the domain, B is called the codomain and 𝑓(𝐴) is called the
range.
Notes
We can show the first representation of function in the form of a table also, which is as follows:
x y
2 4
3 9
4 16
5 25
Of course here the domain and range are discrete and finite subsets of real numbers.
𝑥 2 −9
Now let us consider a function 𝑓(𝑥) = . It is quite clear that the function is not well defined at
𝑥−3
𝑥 = 3, and is good for all other real numbers. Therefore the domain is set of all real numbers except
3. If you input these values of the domain, the function can give any real number as the output,
except 6.
Now we know what happens at 𝑥 = 3, can we just observe the behaviour of the function as 𝑥 goes
closer to 3 from all possible directions? See the following table and see the pattern of 𝑓(𝑥) as 𝑥 goes
close to 3 from left as well as from the right direction.
x f(x)
2.9 5.9
2.99 5.99
2.999 5.999
3.01 6.01
3.001 6.001
3.0001 6.0001
So, you can observe that as 𝑥 is approaching to 3, the 𝑓(𝑥) is approaching to 6. Then we say that the
limit of the function exists at 𝑥 = 3.
Notes
If the function does not approach to the same value from both directions, then we say that the limit
of the function does not exist.
Here it must be mentioned that the word ‘close’ that has been used to define the concept of limit is
not a crisp word. It can mean something to me and entirely different thing to you. This closeness
has to be quantized in order to have a crisp definition of limit and that has been achieved through
the epsilon delta definition.
𝑙𝑖𝑚
1. Prove that 𝑥→−14𝑥 + 1 = −3
𝜖 and you need to find a positive value of 𝛿 for which |𝑓(𝑥) − 𝑙| < 𝜖 whenever 0 < |𝑥 − 𝑐| < 𝛿
holds. This 𝛿 surely depends on 𝜖.
Here we want to find the 𝛿 such that whenever |𝑥 + 1| < 𝛿, |4𝑥 + 1 + 3| < 𝜖 for a predefined 𝜖.
If we work out on the epsilon inequality, we can see |4(𝑥 + 1)| < 𝜖 . That is |𝑥 + 1| < 𝜖/4. Now we can do
𝜖
a smart work here. If we consider 𝜖/4 as 𝛿, we are done. Thus for a given 𝜖 and 𝛿 = , we have |4𝑥 + 1 +
4
3| < 𝜖 whenever |𝑥 + 1| < 𝜖/4.
𝑙𝑖𝑚 1
2. Prove that 𝑥→0 𝑥𝑠𝑖𝑛 ( ) = 0
𝑥
Let 𝜖 > 0 be given. Then we would like to find a 𝛿 > 0, such that
|𝑓(𝑥) − 0| < 𝜖 whenever |𝑥 − 0| < 𝛿
Now
1
|𝑓(𝑥) − 0| = |𝑥𝑠𝑖𝑛 ( )|
𝑥
1
= |𝑥| |sin ( )|
𝑥
≤ |𝑥|
Now choosing 𝛿 = 𝜖 we can see that
|𝑓(𝑥) − 0| < 𝜖 whenever |𝑥| < 𝜖
𝑙𝑖𝑚 1
∴ 𝑥→0 𝑥 sin ( ) = 0
𝑥
Notes Here you can see that the limit of sum of two functions is the sum of their limits. In simple words, you can see
that as 𝑓(𝑥) is getting close to 𝑙 and 𝑔(𝑥) is getting close to 𝑚 as 𝑥 → 𝑎, then 𝑓(𝑥) + 𝑔(𝑥) will go close to
𝑙 + 𝑚 only. Though it can be proved by definition, but here we will resort to common sense only. Similarly
we can see some more properties:
𝑙𝑖𝑚 𝑙𝑖𝑚
𝑥→𝑎 (𝑓 − 𝑔)(𝑥) = 𝑥→𝑎 (𝑓(𝑥) − 𝑔(𝑥)) = 𝑙 − 𝑚
The limit of difference of two functions is the difference in the respective limit of the individual functions.
𝑙𝑖𝑚 𝑙𝑖𝑚
𝑥→𝑎 (𝑓𝑔)(𝑥) = 𝑥→𝑎 𝑓(𝑥)𝑔(𝑥) = 𝑙 𝑚
The limit of the product of two functions is the product of the respective limits of the individual functions.
𝑙𝑖𝑚 (𝑓/𝑔)(𝑥) = 𝑙𝑖𝑚 𝑓(𝑥)/𝑔(𝑥) = 𝑙 /𝑚 (𝑚 ≠ 0)
𝑥→𝑎 𝑥→𝑎
The limit of the quotient of two functions is the quotient of the limits of respective functions.
lim 1−cos 𝑥
3. Evaluate 𝑥→0 𝑥2
𝑥 𝑥 2
1 − cos 𝑥 2 sin2 1 sin 1
lim
= lim 2= lim
( 2
𝑥→0
𝑥2 𝑥→0
𝑥2 𝑥→0
2 𝑥 ) =2
2
lim 𝑒 𝑡𝑎𝑛𝑥 −𝑒 𝑥
4. Evaluate 𝑥→0 tan 𝑥−𝑥
lim 𝑥 lim
Note that 𝑥→0 (1 + 𝑓(𝑥)) = 𝑒 𝑥→0 𝑓(𝑥).𝑥
Now we can modify the given function, so that it takes the form of the left hand side of the above result.
𝑎
𝑙𝑖𝑚 𝑥𝑙𝑜𝑔1+𝑥𝑙𝑜𝑔2+⋯+𝑥𝑙𝑜𝑔𝑛 𝑥
( )
= 𝑒 𝑥→0 𝑛
𝑎
𝑙𝑖𝑚 𝑥𝑙𝑜𝑔 𝑛! 𝑥
𝑥→0 ( )
=𝑒 𝑛
𝑙𝑖𝑚 𝑎𝑥𝑙𝑜𝑔 𝑛!
= 𝑒 𝑥→0 𝑥𝑛
𝑎
= 𝑛! 𝑛
𝑙𝑖𝑚 𝑓(𝑥) = ∞
𝑥→𝑐
A function 𝑓 is said to tend to ∞ as 𝑥 tends to 𝑐, if for any 𝐺 > 0, however large, there corresponds a 𝛿 > 0
such that
Notes
∀ 𝑥 ∈ (𝑐 − 𝛿)𝑈(𝑐, 𝑐 + 𝛿) , 𝑓(𝑥) > 𝐺
𝑙𝑖𝑚 𝑓(𝑥) = −∞
𝑥→𝑐
A function 𝑓 is said to tend to −∞ as 𝑥 tends to 𝑐, if for any 𝐺 > 0, however large, there corresponds a 𝛿 > 0
such that
∀ 𝑥 ∈ (𝑐 − 𝛿)𝑈(𝑐, 𝑐 + 𝛿) , 𝑓(𝑥) < −𝐺
𝑙𝑖𝑚 𝑓(𝑥) = 𝑙
𝑥→∞
A function 𝑓 is said to tend to 𝑙 as 𝑥 tends to ∞, if for any given 𝜖 > 0, there corresponds a 𝐺 > 0 such that
|𝑓(𝑥) − 𝑙| < 𝜖 , ∀ 𝑥 > 𝐺
𝑙𝑖𝑚
𝑥→−∞ 𝑓(𝑥) = 𝑙
A function 𝑓 is said to tend to 𝑙 as 𝑥 tends to −∞, if for any given 𝜖 > 0, there corresponds a 𝐺 > 0 such that
|𝑓(𝑥) − 𝑙| < 𝜖 , ∀ 𝑥 < −𝐺
𝑙𝑖𝑚 𝑓(𝑥) = ∞
𝑥→∞
A function 𝑓 is said to tend to ∞ as 𝑥 tends to ∞, if for any given 𝜖 > 0, there corresponds a 𝐺 > 0 such that
𝑓(𝑥) > 𝜖 , ∀ 𝑥 > 𝐺
𝑙𝑖𝑚 𝑓(𝑥) = ∞
𝑥→−∞
A function 𝑓 is said to tend to ∞ as 𝑥 tends to −∞, if for any given 𝜖 > 0, there corresponds a 𝐺 > 0 such
that
𝑓(𝑥) > 𝜖 , ∀ 𝑥 < −𝐺
𝑙𝑖𝑚
𝑥→∞ 𝑓(𝑥) = −∞
A function 𝑓 is said to tend to −∞ as 𝑥 tends to ∞, if for any given 𝜖 > 0, there corresponds a 𝐺 > 0 such
that
𝑓(𝑥) < 𝜖 , ∀ 𝑥 > 𝐺
𝑙𝑖𝑚 𝑓(𝑥) = −∞
𝑥→−∞
A function 𝑓 is said to tend to −∞ as 𝑥 tends to −∞, if for any given 𝜖 > 0, there corresponds a 𝐺 > 0 such
that
𝑓(𝑥) < 𝜖 , ∀ 𝑥 < −𝐺
1
Let = 𝑦
𝑥
Notes 𝑙𝑖𝑚 1
This implies that 𝑥→0+ 𝑥 =∞
Now consider the case when 𝑥 < 0. This implies that 𝑦 < 0.
Let 𝐺 > 0 be any number, then
1 1
< −𝐺 if − < 𝑥 < 0
𝑥 𝐺
𝑙𝑖𝑚 1
This implies 𝑥→0− = −∞
𝑥
𝑙𝑖𝑚 1
Therefore the left hand limit is different from the right hand limit as 𝑥 is approaching to zero and 𝑥→0 𝑥 does
not exist.
∴ 𝑙𝑖𝑚
𝑥→∞𝑓(𝑥) =2
2𝑥+1 7 7
Again | − 2| = |𝑥−3| < 𝜖 for 𝑥 < − + 3
𝑥−3 𝜖
∴ 𝑙𝑖𝑚
𝑥→−∞𝑓(𝑥) =2
If you look at the definitions of limits at infinity, you can find a positive number 𝐺, in both cases, which
fulfills the required criterion.
𝑙𝑖𝑚
3. Evaluate 𝑥→∞ (√𝑥 2 + 𝑥 + 1 − √𝑥 2 + 1 )
𝑙𝑖𝑚 (√𝑥 2 + 𝑥 + 1 − √𝑥 2 + 1 )
𝑥→∞
𝑙𝑖𝑚
𝑥
= 𝑥→∞
√𝑥 2 + 𝑥 + 1 + √𝑥 2 + 1
𝑙𝑖𝑚
1 1
= 𝑥→∞ =
2
√ 12 + 1 + 1 + √ 12 + 1
𝑥 𝑥 𝑥
L’Hopital Rule
We have got a pretty good idea that for a quotient of two functions, such that the individual limit of
numerator is non-zero and of denominator is zero, then the overall limit of the quotient function
does not exist. In case the individual limit of numerator is zero and that of the denominator is non-
zero, then the overall limit of the quotient function is zero. The third case needs a special attention.
If the individual limit of both numerator as well as the denominator is zero, then this is called one
of the indeterminate forms and there are chances to get its value by using L’Hopital‘s rule.
sin 𝑥
Consider 𝑙𝑖𝑚 . Here the individual limit of the numerator is zero and of the denominator is also
𝑥→0 𝑥
0
zero. This is form. To evaluate this, we will have the following rule (for derivation you can see the
0
link 4 in the last section of the chapter).
Suppose 𝑓 and 𝑔 are differentiable functions over an open interval containing 𝑎, except possibly at
𝑎.
Notes
𝑙𝑖𝑚
If 𝑥→a 𝑙𝑖𝑚
𝑓(𝑥) = 0 and 𝑥→a 𝑙𝑖𝑚
𝑔(𝑥) = 0 then 𝑥→a 𝑙𝑖𝑚
𝑓(𝑥)/g(x) = 𝑥→a 𝑓′(𝑥)/g′(x) assuming the limit on the
right exists or is ∞ or −∞. This result also holds if we are considering one-sided limits, or if 𝑎 = ∞
or 𝑎 = −∞.
sin 𝑥 0
Therefore using the above result for 𝑙𝑖𝑚 as it is a form. We can write the given limit as
𝑥→0 𝑥 0
cos 𝑥
𝑙𝑖𝑚 . And the limit can be evaluated to be one.
𝑥→0 1
0 ∞
There are mainly seven indeterminate forms and we try to convert them in or in form first if
0 ∞
they are not so. And the by the above mentioned formula the limit can be evaluated. Let us see one
more question for better clarity.
Let us evaluate 𝑙𝑖𝑚(𝑥log 𝑥) . Clearly it is 0 ⋅ ∞ form. So first of all we will rewrite the given
𝑥→0
function in the desirable (0/0 or ∞/∞) form.
log 𝑥
𝑙𝑖𝑚(𝑥log 𝑥). = 𝑙𝑖𝑚
𝑥→0 𝑥→01/𝑥
1
= 𝑙𝑖𝑚 𝑥
𝑥→0 1
− 2
𝑥
= 𝑙𝑖𝑚(−𝑥)
𝑥→0
=0
Now let us find the 𝑙𝑖𝑚(cot 𝑥)1/log 𝑥 . Clearly this is an indeterminate form of type ∞0 . First
𝑥→0
of all we will rewrite the given function into the required form. Here you can see the
function as a power of another function. So logarithm can simplify the system.
1
log 𝑦 = log(cot 𝑥)
log 𝑥
log cot 𝑥
⇒ 𝑙𝑖𝑚log 𝑦 = 𝑙𝑖𝑚
𝑥→0 𝑥→0 log 𝑥
−cosec 2 𝑥/ cot 𝑥
= 𝑙𝑖𝑚
𝑥→0 1
𝑥
−𝑥 1
= 𝑙𝑖𝑚 ⋅
𝑥→0 sin 𝑥 cos 𝑥
= −1
⇒ log 𝑙𝑖𝑚𝑦 = −1
𝑥→0
1 1
⇒ 𝑙𝑖𝑚𝑦 = 𝑒 =
𝑥→0 𝑒
Summary
We learnt about the concept of going close to a number from all possible directions. Here we are
dealing with real numbers only so there are only two directions i.e. left and right. The limit of a
function was defined more rigorously using the epsilon delta definition. Since the epsilon delta
definition is tedious to apply, so some properties that can be proved by basic definition come
handy to evaluate the limits of various composite functions. Moreover we learnt the concept of the
limit at infinity and of infinite limits in eight different cases.
Key words
limit, epsilon-delta definition of limit, limit at infinity, infinite limits
Review Questions
1. When do you say that a function 𝑓(𝑥) is approaching to infinity as 𝑥 → ∞?
2. The L’Hopital rule is given as
Notes
𝑓(𝑥) 𝑓′ (𝑥)
𝑙𝑖𝑚 = 𝑙𝑖𝑚
(a) 𝑥→𝑎 𝑔(𝑥) 𝑥→𝑎 𝑔′ (𝑥)
𝑓(𝑥) 𝑓(𝑎)
(b) 𝑙𝑖𝑚 =
𝑥→𝑎 𝑔(𝑥) 𝑔(𝑎)
𝑓(𝑥) 𝑓′ (𝑎)
(c) 𝑙𝑖𝑚 =
𝑥→𝑎 𝑔(𝑥) 𝑔′ (𝑎)
𝑓(𝑥) 𝑓(𝑥)
(d) 𝑙𝑖𝑚 = 𝑙𝑖𝑚[ ]
𝑥→𝑎 𝑔(𝑥) 𝑥→𝑎 𝑔(𝑥)
tan 5𝑥
3. Evaluate 𝑙𝑖𝑚𝜋
𝑥→ 2 tan 𝑥
sin 𝑥
4. 𝑙𝑖𝑚 is
𝑥→0 𝑥
(a) 0 (b) 1 (c) -1 (d) undefined
1 𝑛
5. 𝑙𝑖𝑚 (1 + ) is given as
𝑛→∞ 𝑛
(a) 1 (b) 2 (c) 3 (d) e
1
6. Show that 𝑙𝑖𝑚 =∞
𝑥→0 𝑥 2
Further/Suggested Readings
George B. Thomas Jr., Joel Hass, Christopher Heil & Maurice D. Weir (2018). Thomas’ Calculus
(14th edition). Pearson Education.
Howard Anton, I. Bivens & Stephan Davis (2016). Calculus (10th edition). Wiley India.
https://www.mathsisfun.com/calculus/index.html
https://math.libretexts.org/Bookshelves/Calculus/Map%3A_Calculus__Early_
Transcendentals_(Stewart)/04%3A_Applications_of_Differentiation/4.04%3A_Indeterminate_
Forms_and_l%27Hospital%27s_Rule
Objectives
After studying this unit Students will
Introduction
With the word ‘continuity’, the first thing that comes to our mind is the ability to draw a graph
without lifting the pen.In this unit we will learn when can we tag a function as a continuous
function and if a function is continuous then what more can we know about the function. You will
learn about the various types of discontinuities and the concept of uniform continuity also.
𝑥 2 −1
Examine lim𝑥→1
𝑥−1
1
The right hand limit is lim 1+ 𝑥=
𝑥→ 2
2
1 1
The value of the function at , 𝑓 =1
2 2
The limit of the function is existing but is not equal to the value of the function, so the function is
1 1
not continuous at 𝑥 = . The point 𝑥 = is very much in the domain of the function, so we can say
2 2
that the function is not continuous.
(1) lim
(𝑓 𝑥 + 𝑔(𝑥))is defined, and equals the sum of the values lim 𝑓 𝑥 and lim 𝑔(𝑥).
𝑥→𝑎 𝑥→𝑎 𝑥→𝑎
(3) lim 𝑓(𝑥)𝑔(𝑥) is defined, and equals the product lim 𝑓 𝑥 lim 𝑔(𝑥).
𝑥→𝑎 𝑥→𝑎 𝑥→𝑎
𝑓 𝑥 lim 𝑓 𝑥
lim = 𝑥→𝑎
𝑥→𝑎 𝑔 𝑥 lim 𝑔 𝑥
𝑥→𝑎
The notions of sum, difference, product and quotient of functions can be rewritten as:
lim
(𝑓 + 𝑔) 𝑥 = lim𝑓 𝑥 + lim𝑔 𝑥
𝑥→𝑎 𝑥→𝑎 𝑥→𝑎
lim
(𝑓 − 𝑔) 𝑥 = lim 𝑓 𝑥 − lim𝑔 𝑥
𝑥→𝑎 𝑥→𝑎 𝑥→𝑎
lim
(𝑓. 𝑔) 𝑥 = lim𝑓 𝑥 . lim𝑔 𝑥
𝑥→𝑎 𝑥→𝑎 𝑥→𝑎
You are much familiar with some elementary functions such as the constant function, identity
function, rational function, trigonometric functions, inverse trigonometric functions , exponential
functions and the logarithmic functions.
The domain of continuity of a function is same as the domain of the definition of function.
All the above mentioned elementary functions are continuous in their domain.
For the composed functions, we need to check the continuity every time. Some properties of
continuous functions can be stated as follows.
3𝑥 5 − 4𝑥 2 = 3 on[0,2]
Let 𝑓 𝑥 = 3𝑥 5 − 4𝑥 2 − 3
𝑓(𝑥)is continuous for every 𝑥 as it is a polynomial function.
Now here 𝑓 0 = −3, 𝑓 2 = 77
Let 𝑚 = 3 as 𝑓 0 < 𝑚 < 𝑓(2)
By intermediate value theorem, we can conclude that there exists 𝑐 ∈ [0,2] such that 𝑓 𝑐 = 𝑚
i.e.3𝑐 5 − 4𝑐 2 + 3 = 3
or𝑐 2 3𝑐 3 − 4 = 0
4 1/3
or𝑐 = 0,0,
3
Here all the values of 𝑐 are lying in the given interval. In fact if only one value lies in the interval,
that itself is sufficient to say that the equation is solvable. If we draw the function on 𝑥𝑦 −plane, the
results are quite obvious.
𝑥 2 − 4𝑥 3 + 1 = 𝑥 − 7
Let 𝑓 𝑥 = 𝑥 2 − 4𝑥 3 + 1 − 𝑥 + 7 = −4𝑥 3 + 𝑥 2 − 𝑥 + 8
Here 𝑓 𝑥 is continuous for all 𝑥.
Now in this problem the interval is not given as in the previous example. Therefore by hit and trial
we can look for two values 𝑥 such that the value of the function at those values are of opposite
signs.
𝑥 3 + 2 = 𝑠𝑖𝑛𝑥
Now this equation is a transcendental one. and no interval is given.
Let 𝑓 𝑥 = 𝑥 3 + 2 − sin 𝑥
The function 𝑓 𝑥 is the sum of continuous functions so it is a continuous function for all 𝑥.
𝑓 0 =2
𝑓 −𝜋 = −29
Choosing 𝑚 such that −29 < 𝑚 < 2.
Let 𝑚 = 0
∴ ∃ 𝑐 ∈ −𝜋, 0 such that 𝑓 𝑐 = 𝑚
i.e.𝑐 3 + 2 − sin 𝑐 = 0
Therefore the equation is solvable. And we can verify this by actually plotting the graph which is as
follows:
1. The limit of the functions exists as x tends to c but is different from the value of the
function at c.
2. The limit of the function does not exist at c.
On this basis, we can classify the discontinuities as follows:
1. Removable discontinuity
2. Jump discontinuity (Discontinuity of the first kind)
3. Discontinuity of the first kind from the left
4. Discontinuity of the first kind from the right
5. Discontinuity of the second kind ( Non removable or essential discontinuity)
6. Discontinuity of the second kind from the left
Removable discontinuity
If lim𝑥→𝑐 𝑓 𝑥 exists but is not equal to 𝑓(𝑐) (which may or may not exist), then that discontinuity is
called removable because we can redefine the function so that the function becomes continuous at
point 𝑐.
i.e.lim𝑥 →𝑐 − 𝑓 𝑥 = lim𝑥→𝑐 + 𝑓 𝑥 ≠ 𝑓(𝑐)
sin 𝑥
if 𝑥 ≠ 0
For instance consider the function 𝑓 𝑥 = 𝑥
0 if 𝑥 = 0
Clearly the limit of the function exists and is 1. But the value of the function at 𝑥 = 0 is not 1.
Thus the function has a removable discontinuity at 𝑥 = 0.
It means that we can redefine the function to remove this discontinuity by writing
sin 𝑥
𝑓 𝑥 = if 𝑥 ≠ 0
𝑥
1 if 𝑥 = 0
Jump discontinuity
This discontinuity is also called discontinuity of first kind. If lim𝑥→𝑐 − 𝑓 𝑥 and lim𝑥→𝑐 + 𝑓 𝑥 both
exist but are not equal, then we get a jump discontinuity.
i.e.lim𝑥 →𝑐 − 𝑓 𝑥 ≠ lim𝑥→𝑐 + 𝑓 𝑥
1 if 𝑥 > 0
For instance 𝑓 𝑥 =
−1 if 𝑥 < 0
Clearly the left hand limit is -1 and right hand limit is +1 and you can see a jump right there near
zero, hence the name ‘jump discontinuity’.
𝑥
Consider a function 𝑓 𝑥 = 51−𝑥 2
Clearly the function is not defined at 1 and -1. But we can see how the function will behave as 𝑥
approaches to 1 from both possible directions.
𝑥
The left hand limit = lim𝑥→1− 51−𝑥 2
Put 𝑥 = 1 − . → 0as𝑥 → 1−
So the function can now be written as
𝑥 1−
lim− 51−𝑥 2 = lim 51−(1− )2
𝑥→1 →0
1−
1−h 1
= lim 5 (2− ) (Here tends to as tends to zero.)
→0 2−h 2
1
= lim 52
→0
Therefore in this example the point -1 is a discontinuity of the second kind from the left and 1 is
also a discontinuity of the second kind from the left.
𝑥
Is the function 𝑓 𝑥 = uniformly continuous for 𝑥 ∈ [0,2]?
𝑥+1
𝑥 𝑦 𝑥−𝑦
Now 𝑓 𝑥 − 𝑓 𝑦 = − = ≤ |𝑥 − 𝑦|
𝑥+1 𝑦 +1 𝑥+1 𝑦 +1
1
Show that the function 𝑓 𝑥 = 2 is uniformly continuous on [𝑎, ∞) where 𝑎 > 0, but not
𝑥
uniformly continuous on 0, ∞ .
Let 𝑥, 𝑦 ≥ 𝑎 > 0 be two arbitrary numbers in 0, ∞ .
= 𝑛− 𝑛+1 =1
1 1
And 𝑥1 − 𝑥2 = −
𝑛 𝑛+1
1
=
𝑛 𝑛+1 𝑛+1+ 𝑛
1 1
< = = 𝛿 (say)
𝑛 .2 𝑛 2𝑛
1 1 1
Let 𝜖 = and 𝛿 be any positive number such that 𝑛 > or < 𝛿.
2 2𝛿 2𝑛
Summary
In this unit we have learnt about the technical definition of a continuous function and its various
properties.
lim
(𝑓 − 𝑔) 𝑥 = lim 𝑓 𝑥 − lim𝑔 𝑥
𝑥→𝑎 𝑥→𝑎 𝑥→𝑎
lim
(𝑓. 𝑔) 𝑥 = lim𝑓 𝑥 . lim𝑔 𝑥
𝑥→𝑎 𝑥→𝑎 𝑥→𝑎
Key Words
continuity, discontinuity, intermediate value theorem, uniform continuity
Self Assessment
1. Which of the following is a continuous function?
(a) Constant function
(b) Polynomial function
(c) Sine function
(d) All of the above
2. To verify that any equation is solvable or not, which theorem must be used?
(a) Mean value theorem
(b) Rolle’s theorem
(c) Intermediate value theorem
(d) None of these
3. If a function is continuous, it is definitely uniformly continuous.(True/False)
4. If you can redefine a function so that it becomes continuous, what kind of discontinuity
are you tackling?
(a) Jump
(b) Removable
(c) Discontinuity of first kind
(d) Discontinuity of second kind
𝑥−2
5. lim𝑥→2 is
𝑥 2 −4
(a) 1
(b) 4
1
(c)
4
(d) None of these
6. Which of these functions is not uniformly continuous on (0,1)?
(a) 𝑥 2
𝟏
(b)
𝒙𝟐
(c) sin 𝑥
𝑠𝑖𝑛𝑥
(d)
𝑥
𝑥− 𝑎
7. Find lim𝑥→𝑎 for 𝑏 > 0.
𝑥−𝑎
(a) 0
(b) ∞
(c) 𝑎
1
(d)
2 𝑎
8. Which of the following is not a continuous function?
(a) [𝒙]
Review Questions
1. Prove that a constant function is a continuous function.
2. State the intermediate value theorem with an example.
3. Show that the function 𝑓 𝑥 = 6𝑥 − 5 is continuous at 𝑥 = 0.
4. Discuss the continuity of the following function:
3𝑥 − 5, if 𝑥 ≠ 1
𝑓 𝑥 =
2, if 𝑥 = 1
5. Determine the values of 𝐴 and 𝐵 so that the following function is continuous for all values
of x.
𝐴𝑥 − 𝐵, if 𝑥 ≤ −1
𝑓 𝑥 =
2𝑥 2 + 3𝐴𝑥 + 𝐵, if -1< 𝑥 ≤ 1
and𝑓 𝑥 = 4, if 𝑥 > 1
6. Verify if the equation 𝑥 3 = cos 𝑥 − 2 is solvable or not?
𝑥−5
, if 𝑥 ≠ 5
7. Examine the continuity of 𝑓 𝑥 = 𝑥−5 and discuss in case of any discontinuity.
1, if 𝑥 = 5
𝑥
8. Check if the function is uniformly continuous on 0,2 .
𝑥+2
𝑥−5
, if 𝑥 > 5
9. Examine the continuity of 𝑓 𝑥 = 𝑥−5
1, if 𝑥 ≤ 5
10. Discuss the kind ofdiscontinuity for the following function:
3𝑥 − 5, if 𝑥 ≠ 1
𝑓 𝑥 =
2, if 𝑥 = 1
Further Readings
George B. Thomas Jr., Joel Hass, Christopher Heil& Maurice D. Weir (2018). Thomas’
Calculus (14th edition). Pearson Education.
Howard Anton, I. Bivens& Stephan Davis (2016).Calculus (10th edition).Wiley India.
Web Links
https://math.libretexts.org/Bookshelves/Calculus/Book%3A_Active_Calculus_(Boelkins
_et_al)/1%3A_Understanding_the_Derivative/1.7%3A_Limits_Continuity_and_Differenti
ability
Objectives
Students will
Introduction
After understanding the concept of limit, we can move on to know what is meant by
differentiability of a real valued function. As we know, calculus is all about the study of the change.
The general idea that comes to mind is the average rate of change. We want to say how fast we are,
and to know that, we go for finding the average speed, so if you want to compare two persons, you
just see their average speed or average velocity. Similarly, if you want to see where the bend is
sharper, you would like to see the curvature. To explain the phenomena in more detail, we would
like to know the velocity ‘at a particular point’ or the curvature ‘at a particular point’. Here we are
basically interested in the local change or the instantaneous rate of change. The average rate of
change is kind of global phenomenon, we are telling something for the whole period of time or for
the whole domain in general. In the first case, we need to understand something called
differentiability which is an instantaneous phenomenon or alocal phenomenon.
𝑓(1+ℎ)−𝑓(1) 2ℎ+ℎ2
Now lim = lim = lim 2 + ℎ = 2
ℎ→0 ℎ ℎ→0 ℎ ℎ→0
Clearly the limit does not exist at 𝑥 = 0. Therefor 𝑓 ′ (0) does not exist or we can say that the
modulus function is not differentiable at 𝑥 = 0.
𝑓(𝑥 + ℎ) − 𝑓(𝑥) √𝑥 + ℎ − √𝑥
=
ℎ ℎ
√𝑥+ℎ−√𝑥
(√𝑥 + ℎ + √𝑥)
ℎ
=
√𝑥 + ℎ + √𝑥
1
=
√𝑥 + ℎ + √𝑥
𝑓(𝑥+ℎ)−𝑓(𝑥) 1
Therefore lim = provided 𝑥 > 0 .
ℎ→0 ℎ 2√𝑥
𝑓(0 + ℎ) − 𝑓(0) √ℎ 1
lim = lim = lim
ℎ→0 ℎ ℎ→0 ℎ ℎ→0 √ℎ
1 1
Clearly, lim+ → ∞ and lim− is not defined.
ℎ→0 √ℎ ℎ→0 √ℎ
1
So we can say that 𝑓 ′ (𝑥) = ∀ 𝑥 ∈ (0, ∞)
2√𝑥
𝑓(𝑥) − 𝑓(0) 𝑥2
𝑓 ′ (0+ ) = lim+ = lim+ = lim+𝑥 = 0
𝑥→0 𝑥−0 ℎ→0 𝑥 ℎ→0
is the average rate of change of 𝑦 with respect to 𝑥 over the interval [𝑥, 𝑥 + Δ𝑥]. Now if the graph of
Δ𝑦
𝑦 is a straight line, that is, if 𝑦 = 𝑚𝑥 + 𝑏 for some real numbers 𝑚and 𝑏, then = 𝑚, the slope of
Δ𝑥
Δ𝑦
the line. In fact, a straight line is characterized by the fact is the same for any values of 𝑥and Δ𝑥.
Δ𝑥
Δ𝑦
Moreover, remains the same when Δ𝑥 is infinitesimal; that is, the derivative of 𝑦 with respect to 𝑥
Δ𝑥
Δ𝑦
is the slope of the line. For other differentiable functions 𝑓 , the value of depends upon both 𝑥and
Δ𝑥
Δ𝑦
Δ𝑥 . However, for infinitesimal values of Δ𝑥, the shadow of , that is, the derivative d𝑦
Δ𝑥 d𝑥
, depends on
d𝑦
𝑥 alone. Hence it is reasonable to think of as the slope of the curve 𝑦 = 𝑓(𝑥)at a point𝑥. Whereas
d𝑥
the slope of a straight line is constant from point to point, for other differentiable functions the
value of the slope of the curve will vary from point to point. If 𝑓 is differentiable at a point 𝑎, we
call the line with slope 𝑓′(𝑎)passing through (𝑎, 𝑓(𝑎))the tangent line to the graph of 𝑓at (𝑎, 𝑓(𝑎)).
That is, the tangent line to the graph of 𝑦 = 𝑓(𝑥) at 𝑥 = 𝑎 is the line with equation
𝑦 = 𝑓 ′ (𝑎) (𝑥 − 𝑎) + 𝑓(𝑎)
Hence a tangent line to the graph of a function 𝑓 is a line through a point on the graph of 𝑓whose
slope is equal to the slope of the graph at that point.
The third and fourth derivatives of distance w.r.t. time are called jerk and jounce.
𝑎(𝑡+Δ𝑡)−𝑎(𝑡) Δ𝑎 𝑑𝑎
lim = lim ( ) = = jerk (j) at time 𝑡
Δ𝑡→0 Δ𝑡 Δ𝑡→0 Δ𝑡 𝑑𝑡
𝑗(𝑡+Δ𝑡)−𝑗(𝑡) Δ𝑗 𝑑𝑗
lim = lim ( ) = = jounce (J) at time 𝑡
Δ𝑡→0 Δ𝑡 Δ𝑡→0 Δ𝑡 𝑑𝑡
You can see and feel all these changes physically in the real world. But that will not be the case with
all the functions other than the distance function.
The derivative of various functions have been developed through the ab-initio definition. Two
examples are given.
= 𝑓 ′ (𝑐) ∗ 0 = 0
∴ lim 𝑓(𝑐 + h) − 𝑓(𝑐) = 0
ℎ→0
Alternatively,
lim 𝑓(𝑥) = 𝑓(𝑐)
𝑥→𝑐
We can recall that for an increasing function 𝑥1 < 𝑥2 ⇒ 𝑓(𝑥1 ) < 𝑓(𝑥2 ) and for a decreasing function
𝑥1 < 𝑥2 ⇒ 𝑓(𝑥1 ) > 𝑓(𝑥2 ). The functions which are increasing as well as decreasing in their domain
are known as non-monotonic functions. For example the absolute function, the sine function etc.
Monotonicity in an interval
For an increasing function in some interval if Δ𝑥 > 0 ⇔ Δ𝑦 > 0or Δ𝑥 < 0 ⇔ Δ𝑦 < 0, then the
function is said to be strictly monotonically increasing in that interval.
𝑑𝑦
i.e. if > 0 in some interval then 𝑦 is said to be a strictly increasing function in that interval.
𝑑𝑥
𝑑𝑦
Similarly, if < 0 in some interval then 𝑦 is said to be a strictly decreasing function in that interval.
𝑑𝑥
𝑑𝑦 𝑑𝑦
if ≥ 0 in some interval then 𝑦 is said to be a increasing function in that interval. Similarly, if ≤
𝑑𝑥 𝑑𝑥
0 in some interval then 𝑦 is said to be a decreasing function in that interval.
𝑓(𝑥) = 𝑥 − sin 𝑥
𝑓′(𝑥) = 1 − cos 𝑥
𝑓 ′′ (𝑥) ≥ 0 ∀ 𝑥 ∈ 𝑹
Therefore 𝑓(𝑥) is monotonically increasing ∀ 𝑥 ∈ 𝑹
Find the interval in which the function 𝑓(𝑥) = 2𝑥 2 − ln |𝑥| is (i) decreasing (ii) increasing.
𝑓(𝑥) = 2𝑥 2 − ln|𝑥|
1 4𝑥 2 − 1
𝑓 ′ (𝑥) = 4𝑥 − =
x 𝑥
Domain of the function is(0, ∞). Therefore the denominator of 𝑓 ′ (𝑥) is always positive and
numerator has all the power to decide.
For 𝑓(𝑥) to be decreasing
𝑓 ′ (𝑥) ≤ 0
4𝑥 2 − 1 ≤ 0
1
𝑥2 ≤
4
1
|𝑥| ≤
2
1 1
− ≤𝑥≤
2 2
1
𝑥 ∈ (0, ]
2
For 𝑓(𝑥) to be increasing
1
• From onwards the function is increasing
2
1
• In (0, ] the function is decreasing.
2
1
• At the function is having a minimum value.
2
Summary
In this unit we have learnt the basic definition of differentiability and its geometric and kinematic
interpretations. We have learnt some results related to differentiability with continuity and
monotonicity. The following are the main point:
𝑓(𝑐+ℎ)−𝑓(𝑐)
• To check the derivability, we need to check if the limit lim exists or not.
ℎ→0 ℎ
• If f is finitely derivable at c, then f is also continuous at c.
• If a function is monotonically increasing at 𝑥 = 𝑎, its first derivative at 𝑥 = 𝑎 has to be
positive and if a function is monotonically decreasing at 𝑥 = 𝑎, its first derivative at 𝑥 = 𝑎
has to be negative.
Key Words
• Differentiability
• Derivability
• Differentiability and continuity
• Differentiability and monotonicity
Self Assessment
1. Which of the following does not lead to the idea of differentiability?
A. instantaneous rate of change
11. Which of the following function is continuous and not differentiable in its domain?
A. 𝑥 2
B. √𝑥
C. |𝑥|
1
D.
𝑥
15. Which of the following suggests that the function is strictly decreasing?
A. 𝑥1 < 𝑥2 implies 𝑓(𝑥1 ) < 𝑓(𝑥2 )
B. 𝑥1 < 𝑥2 implies 𝑓(𝑥1 ) > 𝑓(𝑥2 )
C. 𝑥1 < 𝑥2 implies 𝑓(𝑥1 ) ≤ 𝑓(𝑥2 )
D. 𝑥1 < 𝑥2 implies 𝑓(𝑥1 ) ≥ 𝑓(𝑥2 )
17. The functions which are increasing as well as decreasing in their domain are known as
A. increasing functions
B. decreasing functions
C. monotonic functions
D. non monotonic functions
6. C 7. B 8. D 9. A 10. A
Review Questions
1. Find the derivative of 𝑓(𝑥) = 2𝑎𝑥 + 𝑏 using first principle.
1
2. Find the derivative of 𝑓(𝑥) = using first principle.
𝑥 2 +3
3. Discuss the differentiability of the function (𝑥) = |𝑥 − 2| + |𝑥| + |𝑥 + 2| .
4. Find the slope of the tangents to the parabola 𝑦 = 𝑥 2 at points (2, 4) and (-1, 1).
5. Find the interval in which the function 𝑓(𝑥) = 3𝑥 2 − ln |𝑥| is (i) decreasing (ii) increasing.
6. Find the interval in which the function 𝑓(𝑥) = log 𝑥 + 𝑥 is (i) decreasing (ii) increasing.
1 1
𝑥(𝑒 − 𝑥 −𝑒 𝑥 )
7. Examine 𝑓(𝑥) = { 1 1 𝑥 ≠ 0 for the continuity and differentiability at origin.
𝑒 − 𝑥 +𝑒 𝑥
1 𝑥=0
8. Find the interval in which the function 𝑓(𝑥) = 𝑥 − cos 𝑥 is (i) decreasing (ii) increasing.
9. Find the derivative of hyperbolic sine function using ab initio method.
10. Design a function which is increasing on some part of the domain and decreasing on
other. Then discuss the differentiability and continuity of that function.
Further Readings
George B. Thomas Jr., Joel Hass, Christopher Heil& Maurice D. Weir (2018). Thomas’
Calculus (14th edition). Pearson Education.
Howard Anton, I. Bivens& Stephan Davis (2016). Calculus (10th edition). Wiley India.
A Geometric Interpretation of the Derivatives. (2020, November 17). Retrieved May 4,
2021, from https://math.libretexts.org/@go/page/25429
Web Links
https://math.libretexts.org/Bookshelves/Calculus/Book%3A_Active_Calculus_(Boelkins
_et_al)/1%3A_Understanding_the_Derivative/1.7%3A_Limits_Continuity_and_Differenti
ability
Objectives
Students will
• learn about the derivative of the function of function
• explore the property of a differentiable function called Darboux’s theorem
• learn to apply the Rolle’s theorem
Introduction
If the function is made up of functions called composed functions or a composite function, then
what to do in case, if we are interested in the derivative of a composed function! This question will
be answered in this unit. The derivative of function of function is popularly known as the chain rule
of differentiation.
Let 𝑓 and 𝜙 be two derivable functions such that 𝑦 = 𝑓(𝑢)and 𝑢 = 𝜙(𝑥). Clearly you can see that 𝑦
is a function of 𝑢 and 𝑢 is a function of 𝑥 and ultimately 𝑦 is a function of 𝑥.
𝑦 𝑢 𝑥
The range of 𝜙 must be a subset of the domain of 𝑓, then only we would be able to write 𝑦 =
𝑓(𝜙(𝑥)) which is also called the composite function. Moreover we know that
(𝑓𝑜𝜙)(𝑥) = 𝑓(𝜙(𝑥))
Δ𝑦 Δ𝑦 Δ𝑢
lim = lim . lim
Δ𝑥→0 Δ𝑥 Δ𝑥→0 Δ𝑢 Δ𝑥→0 Δ𝑥
𝑑𝑦 𝑑𝑦 𝑑𝑢
= .
𝑑𝑥 𝑑𝑢 𝑑𝑥
Let us understand the rule better with the following examples:
𝑢 = 1 + 𝑥 2 , 𝑦 = √𝑢; then𝑦 = √1 + 𝑥 2
𝑑𝑢
Now = 2𝑥
𝑑𝑥
𝑑𝑦 1 −1 1 1
= 𝑢 2 = (1 + 𝑥 2 )−2
𝑑𝑢 2 2
𝑑𝑦 𝑑𝑦 𝑑𝑢 𝑥
Therefore, = . = .
𝑑𝑥 𝑑𝑢 𝑑𝑥 √1+𝑥 2
We can look at the same problem by layers’ point of view. The square root is the outer layer , it has
to be dealt with first and then the polynomial as the inner layer will be considered. We can write it
as
1+𝑥
Find the derivative of the function √ .
1−𝑥
1
1+𝑥
Let = 𝑢, then 𝑦 = √𝑢 = 𝑢2
1−𝑥
1
𝑑𝑦 1 −1 1 1 + 𝑥 −2
= 𝑢 2 = .( )
𝑑𝑢 2 2 1−𝑥
𝑑𝑢 2
=
𝑑𝑥 (1 − 𝑥)2
1 1
𝑑𝑦 1 1 + 𝑥 −2 2 (1 + 𝑥)−2
= ( ) . = 3
𝑑𝑥 2 1 − 𝑥 (1 − 𝑥)2 (1 − 𝑥)2
𝑑𝑥
= cosh 𝑦
𝑑𝑦
𝑑𝑦 1
⇒ =
𝑑𝑥 cosh 𝑦
1
=±
√(1 + sinh2 𝑦)
1
=±
√1 + 𝑥 2
The sign of the radical must be same as that of cosh 𝑦.
𝑑𝑦 1
Therefore, =
𝑑𝑥 √1+𝑥 2
−1 𝑥
Find the derivative of the function 𝑒 𝑠𝑖𝑛ℎ .
Let 𝑦 = sinh−1 𝑥
−1
𝑑𝑦 𝑑(𝑒 𝑠𝑖𝑛ℎ 𝑥 ) 𝑑(sinh−1 𝑥)
= .
𝑑𝑥 𝑑(sinh−1 𝑥) 𝑑𝑥
−1 𝑥 1
= 𝑒 sinh .
√1 + 𝑥 2
Find the maximum and minimum values of 𝑓(𝑥) = sin 𝑥 + cos 𝑥 on [0, 2𝜋].
The function is continuous on [0, 2𝜋].
𝑓 ′ (𝑥) = cos 𝑥 − sin 𝑥
𝜋 5𝜋
The critical points are ( , √2)and ( , −√2). The function values at the end pointsof the given
4 4
interval are 𝑓(0) = 1and 𝑓(2𝜋) = 1.
Proof
Consider the function
ℎ(𝑥) = 𝑓(𝑥) − (𝑓(𝑏) + 𝑟(𝑥 − 𝑏))
Because 𝑓(𝑥) is differentiable, it is definitely continuous.
𝑓(𝑏) + 𝑟(𝑥 − 𝑏) is also continuous and differentiable.
∴ ℎ(𝑥)is continuous and differentiable on [𝑎, 𝑏].
Thus if f is differentiable on the closed interval [a, b] and r is any number between f ’(a) and f ’ (b),
then there exists a number c in the open interval (a, b) such that f ‘ (c) = r.
Jean Gaston Darboux was a French mathematician who lived from 1842 to 1917. Of his
several important theorems the one we just studied says that the derivative of a function has the
Intermediate Value Theorem property – that is, the derivative takes on all the values between the
values of the derivative at the endpoints of the interval under consideration.
Another interesting aspect of Darboux’s Theorem is that there is no requirement that the derivative
f ‘(x) be continuous!
1
The common example of such a function is𝑓(𝑥) = 𝑥 2 sin when 𝑥 ≠ 0 and 𝑓(𝑥) = 0 when 𝑥 = 0
𝑥
1 1
With𝑓 ′ (𝑥) = 2𝑥 sin − cos , 𝑥 ≠ 0
𝑥 𝑥
This function is differentiable and hence continuous. There is an oscillating discontinuity at the
origin. The derivative is not continuous at the origin. Yet, every interval containing the origin as an
interior point meets the conditions of Darboux’s Theorem, so the derivative while not being
continuous has the intermediate value property.
Proof
In the statement of Rolle's theorem, f(x) is a continuous function on the closed interval [a,b]. Hence
by the Intermediate Value Theorem it achieves a maximum and a minimum on [a,b]. Either one of
these occurs at a point c with a < c < b,
Since f(x) is differentiable on (a,b) and c is an extremum we then conclude that f '(c) = 0.
or both the maximum and minimum occur at endpoints.
Since f(a) = f(b), this means that the function is never larger or smaller than f(a). In other words, the
function f(x) is constant on the interval [a,b] and its derivative is therefore 0 at every point in (a,b).
Hence proved
Geometric interpretation
There is a point c on the interval (a,b)where the tangent to the graph of the function is parallel to
the x-axis.
This property was known in the 12th century in ancient India. The outstanding Indian
astronomer and mathematician Bhaskara II mentioned it in his writings.
For instance, consider𝑓(𝑥) = |𝑥| (where |𝑥|is the absolute value of 𝑥 on the closed interval [-1,1].
This function does not have derivative at= 0. Though f(x) is continuous on the closed interval [-1,1]
there is no point inside the interval (−1,1)at which the derivative is equal to zero. The Rolle’s
Theorem fails here because𝑓(𝑥) is not differentiable over the whole interval(−1,1).
⇒ 𝑐=0
And 0 ∈ (−1,1)
Thus the Rolle’s Theorem gets verified.
𝑥
Verify Rolle’s theorem for 𝑓(𝑥) = 𝑥(𝑥 + 3)𝑒 −2 in [−3,0].
The function is a product of continuous functions, therefore it is continuous in [−3,0].
The function is differentiable in (−3,0). (solve for the derivative of the function and check if it exists
in (−3,0), It will be!)
𝑓(−3) = 𝑓(0)
Therefore there will exist a point 𝑐 , such that𝑓 ′ (𝑐) = 0.
Or 𝑐 2 − 𝑐 − 6 = 0
Or 𝑐 = −2, 3
Thus we got at least a point −2 ∈ (−3,0).
Thus Rolle’s theorem gets verified for the given function in the given interval.
Summary
This unit is an extension of the differentiability to a function of a function. We have understood and
learnt the formulae of the derivatives of elementary functions already.
• In order to differentiate a composite function, of course those formulae will not be
applicable directly. We need to use the chain rule.
𝑑
• (𝑓(𝜙(𝑥)) = 𝑓 ′ (𝜙(𝑥))𝜙′(𝑥)
𝑑𝑥
• A significant result for a differentiable function on a closed interval, given as,
If f is differentiable on the closed interval [a, b] and r is any number between f ’(a) and
f ’ (b), then there exists a number c in the open interval (a, b) such that f ‘ (c) = r.
• Rolle’s theorem states that ‘If f(x) is continuous an [a,b] and differentiable on (a,b) and if
f(a) = f(b) then there is some c in the interval (a,b) such that f '(c) = 0.’
Key Words
chain rule, derivative of a function of function, extreme value theorem, Darboux’s theorem, Rolle’s
theorem
Self Assessment
1. The derivative of the function √2 + 𝑥 2 is
𝑥
A. 2
2√2+𝑥
𝑥
B.
√2+2𝑥 2
𝑑
2. (𝑠𝑖𝑛(𝑐𝑜𝑠𝑥)) =
𝑑𝑥
A. sin 𝑥 cos (cos 𝑥)
B. cos (sin 𝑥)
C. −sin 𝑥 cos (cos 𝑥)
D. sin 𝑥 cos (sin 𝑥)
3. If f is differentiable on the closed interval [a, b] and r is any number between f ’ (a) and
f ’(b), then there exists a number c in the open interval (a, b) such that f ’(c) = r. This
statement is of
A. intermediate value theorem
B. mean value theorem
C. Rolle’s theorem
D. Darboux’s theorem
−1 𝑥
𝑒 𝑠𝑖𝑛ℎ
4. is the derivative of the function
√1+𝑥 2
−1
𝑒 𝑠𝑖𝑛ℎ 𝑥
A. x
√1+𝑥 2
−1
𝑒 𝑠𝑖𝑛ℎ 𝑥
B.
√1+𝑥 2
−1
C. 𝑒 𝑠𝑖𝑛ℎ 𝑥 ans
−1
D. 𝑒 𝑐𝑜𝑠ℎ 𝑥
𝑑 𝑠𝑖𝑛𝑥
6. 𝑒 =
𝑑𝑥
A. 𝑒 𝑠𝑖𝑛𝑥
cos 𝑥
B. cos (sin 𝑥)
C. − 𝑒 𝑠𝑖𝑛𝑥 cos 𝑥
D. sin 𝑥 cos (sin 𝑥)
7. If a function 𝑓 is
I. continuous on [𝑎, 𝑏]
II. derivable on (𝑎, 𝑏)
III. 𝑓(𝑎) = 𝑓(𝑏)
IV. then there exists one value 𝑐 ∈ (𝑎, 𝑏) such that 𝑓 ′ (𝑐) = 0
Which of the following are correct for 𝑓 to satisfy the Rolle’s Theorem?
A. I, II and III
B. I, II and IV
C. II, III and IV
D. III and IV
𝑥
9. The function 𝑓(𝑥) = 𝑥(𝑥 + 3)𝑒 −2 in [−1, 1] satisfies the Rolle’s Theorem.
A. True
B. False
10. For all the second degree polynomials 𝑦 = 𝑎𝑥 2 + 𝑏𝑥 + 𝑘, it is seen that the Rolles’ point is
at 𝑐 = 0. Also the value of 𝑘 is zero. Then what is the value of 𝑏?
11. If 𝑓 is continuous function on the closed interval [𝑎, 𝑏], and 𝑁 is a number between 𝑓(𝑎)
and 𝑓(𝑏), then there is 𝑐 ∈ [𝑎, 𝑏]such that 𝑓(𝑐) = 𝑁 is:
A. The Intermediate Value Theorem
B. The Mean Value Theorem
C. Rolle's Theorem
D. The Extreme Value Theorem
12. According to Rolle's theorem, for a differentiable function f(x), if the start point f(a) and
the end point f(b) equal 0 then:
A. Rolle's Theorem does not apply.
B. Somewhere between f(a) and f(b) the instantaneous rate of change must be 0.
C. Somewhere between f(a) and f(b) the function must equal 0.
D. The function is flat.
6. A 7. A 8. B 9. B 10. A
11. A 12. B
Review Questions
1. Find the derivative of the function 𝑓(𝑥) = sin(√𝑥 2 − 5)
√1−𝑥
2. Find the derivative of the function 𝑓(𝑥) =
1+𝑥
3. Find the derivative of the function 𝑓(𝑥) = sin ℎ(√𝑥 2 + 5)
4. Find the derivative of the function 𝑓(𝑥) = log (cosh 𝑒 𝑥 )
𝑥
5. Find the derivative of the function 𝑓(𝑥) = 2(cosh 𝑒 )
6. Find the derivative of the function 𝑓(𝑥) = tan 𝑥−1
Further Reading
George B. Thomas Jr., Joel Hass, Christopher Heil & Maurice D. Weir (2018). Thomas’
Calculus (14th edition). Pearson Education.
Howard Anton, I. Bivens& Stephan Davis (2016).Calculus (10th edition).Wiley India.
https://www.math.ucdavis.edu/~kouba/CalcOneDIRECTORY/chainruledirectory/Chain
Rule.html
https://www.cliffsnotes.com/study-guides/calculus/calculus/the-derivative/chain-rule
https://www.cliffsnotes.com/study-guides/calculus/calculus/applications-of-the-
derivative/extreme-value-theorem
https://www.math24.net/rolles-theorem
Objectives
Students will
• learn about the properties of a differentiable function
• understand the basics of Lagrange’s mean value theorem
• be able to use Cauchy’s mean value theorem
• be able to interpret the mean value theorems geometrically
Introduction
If a function is appropriately differentiable and continuous then it can lead to much more
information about the nature and behavior of the function. In this chapter we will learn the more
general form of the Rolle’s Theorem and then the general form of the Lagrange mean value
theorem with their physical interpretations.
Proof
Define a new function
𝜙(𝑥) = 𝑓(𝑥) + 𝐴𝑥, 𝑥 ∈ [𝑎, 𝑏]
We choose a number 𝐴 such that the condition 𝜙(𝑎) = 𝜙(𝑏) is satisfied. Then
𝑓(𝑎) + 𝐴𝑎 = 𝑓(𝑏) + 𝐴𝑏
𝑓(𝑏) − 𝑓(𝑎)
𝐴=−
𝑏−𝑎
As a result, we have
or
𝑓(𝑎 + ℎ) = 𝑓(𝑎) + ℎ 𝑓 ′ (𝑎 + 𝜃ℎ), 𝜃 ∈ (0,1)
If 𝑓(𝑥) = (𝑥 − 1)(𝑥 − 2)(𝑥 − 3), 𝑥 ∈ [0,4], find 𝑐 such that the average rate of change of 𝑓(𝑥)
is equal to the derivative of f(x) at 𝑐.
Here,
𝑓(0) = −6
𝑓(4) = 6
𝑓(4)−𝑓(0)
So, =3
4−0
Also 𝑓 ′ (𝑥) = 3𝑥 2 − 12 𝑥 + 11
According to the statement,
𝑓(4) − 𝑓(0)
= 𝑓′(𝑐)
4−0
3𝑐 2 − 12𝑐 + 11 − 3 = 0
6 ± 2√3
⇒ 𝑐=
8
𝑏 2 + 𝑎𝑏 + 𝑎2
𝑐 = ±√
3
Prove that for any quadratic function 𝑝𝑥 2 + 𝑞𝑥 + 𝑟, the value of 𝜃 in Lagrange’s theorem is
1
always , for any 𝑝, 𝑞, 𝑟, 𝑎, ℎ.
2
If in the Cauchy’s mean value theorem 𝑓(𝑥) = 𝑒 𝑥 and 𝐹(𝑥) = 𝑒 −𝑥 , show that 𝑐 is the
arithmetic mean between 𝑎 and 𝑏.
Here 𝑓 ′ (𝑥) = 𝑒 𝑥
𝐹 ′ (𝑥) = −𝑒 −𝑥
By Cauchy’s mean value theorem,
𝑓 ′ (𝑐) 𝑓(𝑏) − 𝑓(𝑎)
=
𝐹′(𝑐) 𝐹(𝑏) − 𝐹(𝑎)
𝑒𝑐 𝑒𝑏 − 𝑒𝑎
=
−𝑒 −𝑐 𝑒 −𝑏 − 𝑒 −𝑎
−𝑒 2𝑐 = −𝑒 𝑎+𝑏
This implies
𝑎+𝑏
𝑐=
2
𝑠𝑖𝑛𝛼−𝑠𝑖𝑛𝛽 𝜋
Show that = cot 𝜃, 0<𝛼<𝜃<𝛽<
𝑐𝑜𝑠𝛽−𝑐𝑜𝑠𝛼 2
Looking at the result to be proved, you can see that the left hand side is a ratio of difference of two
functions and Cauchy’s theorem can be used to derive this, provided these two functions satisfy the
requirements of Cauchy’s mean value theorem.
Let 𝑓(𝑥) = sin 𝑥
𝐹(𝑥) = cos 𝑥 𝑥 ∈ [𝛼, 𝛽]
𝑓′(𝑥) = cos 𝑥
𝐹′(𝑥) = −sin 𝑥
By Cauchy’s mean value theorem we can write,
𝑓(𝛽) − 𝑓(𝛼) 𝑓 ′ (𝜃)
=
𝐹(𝛽) − 𝐹(𝛼) 𝐹 ′ (𝜃)
𝑠𝑖𝑛𝛽 − 𝑠𝑖𝑛𝛼 cos 𝜃
=
cos 𝛽 − cos 𝛼 −𝑠𝑖𝑛𝜃
𝑠𝑖𝑛𝛽 − 𝑠𝑖𝑛𝛼
= − cot 𝜃
cos 𝛽 − cos 𝛼
or
𝑠𝑖𝑛𝛼 − 𝑠𝑖𝑛𝛽
= cot 𝜃
cos 𝛽 − cos 𝛼
Hence the result
Check the validity of Cauchy’s mean value theorem for the functions 𝑓(𝑥) = 𝑥 4 and 𝑔(𝑥) =
𝑥 on the interval[1,2].
2
Here
𝑓(𝑥) = 𝑥 4
𝑓′(𝑥) = 4𝑥 3
𝑔(𝑥) = 𝑥 2
𝑔′(𝑥) = 2𝑥
Both functions are satisfying all the criteria of continuity and differentiability, therefore we can
write
𝑓 ′ (𝑐) 𝑓(𝑏) − 𝑓(𝑎)
=
𝑔′(𝑐) 𝑔(𝑏) − 𝑔(𝑎)
4𝑐 3 𝑏 4 − 𝑎4
= 2
2𝑐 𝑏 − 𝑎2
2𝑐 2 = 𝑎2 + 𝑏 2
Here 𝑎 = 1, 𝑏 = 2
Summary
This unit is an extension of the Rolle’s Theorem. Its generalized form can be seen as Lagrange’s
mean value theorem, which further can be generalized as the Cauchy’s mean value theorem.
• Lagrange’s mean value theorem (MVT) states that if a function 𝑓(𝑥) is continuous on a
closed interval [𝑎, 𝑏]and differentiable on the open interval (𝑎, 𝑏), then there is at least one
𝑓(𝑏)−𝑓(𝑎)
point 𝑥 = 𝑐 on this interval, such that = 𝑓′(𝑐).
𝑏−𝑎
Key Words
Lagrange’s mean value theorem, Cauchy’s mean value theorem
Self Assessment
on the interval[4, 5].
𝑥−1
1. The Lagrange’s mean value theorem is valid for the function 𝑓(𝑥) =
𝑥−3
A. True
B. False
2. All points c satisfying the conditions of the MVT for the function 𝑓(𝑥) = 𝑥 3 − 𝑥in the interval
[−2, 1] are
A. -1
B. 1, -1
C. 0
D. 1
3. For any quadratic function𝑝𝑥 2 + 𝑞𝑥 + 𝑟, the value of 𝜃 in Lagrange’s theorem, for any
𝑝, 𝑞, 𝑟, 𝑎, ℎ is
A. less than ½
B. greater than ½
C. always ½
D. can take any value
A. 0
B. 1
C. 0.5
D. 1.5
5. Cauchy’s Mean Value Theorem can be reduced to Lagrange’s Mean Value theorem.
A. True
B. False
6. Which of the following is not a necessary condition for Cauchy’s Mean Value Theorem?
7. Cauchy’s Mean Value Theorem is also known as ‘Extended Mean Value Theorem’.
A. True
A. Leonhard Euler
B. Govindasvami
C. Michel Rolle
D. Augustin Louis Cauchy
9. The value of c which satisfies the Mean Value Theorem for the function 𝑓(𝑥) = 𝑥 2 + 2𝑥 + 1 on
[1,2] is
A. -5/2
B. -5/2
C. 7/2
D. -7/2
10. What is the value of c which lies in [1, 2] for the function f(x)= 4x and g(x)= 3x 2?
A. 1
B. 1.5
C. 2
D. 2.5
6. B 7. A 8. D 9. D 10. B
Review Questions
1. State and prove the Lagrange’s mean value theorem.
2. State and prove the Cauchy’s mean value theorem.
3. Check the validity of Cauchy’s MVT for the functions f(x)= 4x and g(x)= 3x2
4. Check the validity of Lagrange’s MVT for the function 𝑓(𝑥) = 𝑥 2 + 2𝑥 + 1 on [1,2].
5. Check the validity of Lagrange’s MVT for the function 𝑓(𝑥) = 𝑥 2 + 2𝑥 + 1 on [-1,2].
6. Explain how the Lagrange’s MVT is a special case of Cauchy’s MVT.
7. Discuss the Lagrange’s MVT in the interval [𝑎, 𝑎 + ℎ].
8. Discuss the Cauchy’s MVT in the interval [𝑎, 𝑎 + ℎ].
Further Reading
George B. Thomas Jr., Joel Hass, Christopher Heil& Maurice D. Weir (2018). Thomas’
Calculus (14th edition). Pearson Education.
Howard Anton, I. Bivens& Stephan Davis (2016).Calculus (10th edition).Wiley India.
https://www.math24.net/cauchys-mean-value-theorem
https://www.geeksforgeeks.org/lagranges-mean-value-theorem
https://tutorial.math.lamar.edu/classes/calci/MeanValueTheorem.aspx
Objectives
Students will
Introduction
By now, we have a good idea about what is differentiation, we
know the technique how to differentiate a function, we have
derived quite a few rules of the derivatives for some functions
also. Continuing the stride, we now look into how the higher
derivatives can be found out in a general manner. We will
discuss how to find the nth derivative for some specific
functions in this chapter. We will see the process of
differentiating a given function successively n times, which is
known as successive differentiation and the results that you get
are called successive derivatives.
and so on
For instance, 𝑓(𝑥) = 𝑥 5 + sin 𝑥 + 𝑒 2𝑥
𝑓 ′ (𝑥) = 5𝑥 4 + cos 𝑥 + 2𝑒 2𝑥
𝑓 ′′ (𝑥) = 20𝑥 3 − sin 𝑥 + 4𝑒 2𝑥
𝑓 ′′′ (𝑥) = 60𝑥 2 − cos 𝑥 + 8 𝑒 2𝑥
and so on.
1
Find the 𝑛𝑡ℎ derivative of .
1−5𝑥+6𝑥 2
Now here the given function is a composite function. We can work out on the function to write it as
an elementary function whose 𝑛𝑡ℎ derivative is known.
1
Let 𝑦 =
1−5𝑥+6𝑥 2
1
=
(1 − 3𝑥)(1 − 2𝑥)
3 2
= −
1 − 3𝑥 1 − 2𝑥
1
Now these two expressions are of the form . Working out on the 𝑛𝑡ℎ derivative of this function
𝑎𝑥+𝑏
(−1)𝑛 𝑛!𝑎𝑛
we get (𝑎𝑥+𝑏)𝑛+1
Applying the direct result of the sine and cosine functions, we get
1 𝑛𝜋 𝑛𝜋
𝑦𝑛 = (10𝑛 sin (10𝑥 + ) + 2𝑛 cos (2𝑥 + ))
2 2 2
𝑑2𝑦
If 𝑦 = 𝑥 + tan 𝑥, show that cos2 𝑥 − 2𝑦 + 2𝑥 = 0
𝑑𝑥 2
1
𝑢2 = −
𝑥2
2
𝑢3 = 3
𝑥
2.3
𝑢4 = − 4
𝑥
⋮
(−1)𝑛−1 (𝑛 − 1)!
𝑢𝑛 =
𝑥𝑛
Let 𝑣 = 𝑥
𝑣1 = 1
𝑣2 = 0
𝑣3 = 0
⋮
𝑣𝑛 = 0
By Leibnitz theorem,
(𝑢𝑣)𝑛 = 𝑢𝑛 𝑣 + 𝑛1𝐶 𝑢𝑛−1 𝑣1 + 𝑛2𝐶 𝑢𝑛−2 𝑣2 + ⋯ + 𝑛𝑟𝐶 𝑢𝑛−𝑟 𝑣𝑟 + ⋯ + 𝑢𝑣𝑛
(−1)𝑛−1 (𝑛 − 1)! 𝑛(−1)𝑛−2 (𝑛 − 2)!
(𝑥𝑙𝑜𝑔𝑥)𝑛 = +
𝑥 𝑛−1 𝑥 𝑛−1
(−1)𝑛−2 (𝑛 − 2)!
=
𝑥 𝑛−1
If 𝑦 = tan−1 𝑥, show that (1 + 𝑥 2 )𝑦𝑛+2 + 2(𝑛 + 1)𝑥𝑦𝑛+1 + 𝑛(𝑛 + 1)𝑦𝑛 = 0. Also find 𝑦𝑛 (0).
Here 𝑦 = tan−1 𝑥
1
𝑦1 =
1 + 𝑥2
⇒ (1 + 𝑥 2 )𝑦1 = 1
Summary
This chapter is about the higher derivative of a function. We also learnt about how to find the nth
derivative of the product of two functions.
• The process of differentiating a given function successively n times are called successive
differentiation and the results of such differentiation are called successive derivatives.
• If u and v are functions of x such that their 𝑛𝑡ℎ derivatives exist, then the 𝑛𝑡ℎ derivative of
their product is given by
(𝑢𝑣)𝑛 = 𝑢𝑛 𝑣 + 𝑛1𝐶 𝑢𝑛−1 𝑣1 + 𝑛2𝐶 𝑢𝑛−2 𝑣2 + ⋯ + 𝑛𝑟𝐶 𝑢𝑛−𝑟 𝑣𝑟 + ⋯ + 𝑢𝑣𝑛
where𝑢𝑟 and 𝑣𝑟 represent the 𝑟 𝑡ℎ derivatives of 𝑢 and 𝑣 respectively.
Self Assessment
1. The derivative of the function √2 + 𝑥 2 is
𝑥
A. 2
2√2+𝑥
𝑥
B.
√2+2𝑥 2
2𝑥
C.
√2+𝑥 2
𝑥
D.
√2+𝑥 2
𝑑
2. (𝑠𝑖𝑛(𝑐𝑜𝑠𝑥)) =
𝑑𝑥
A. sin 𝑥 cos (cos 𝑥)
B. cos (sin 𝑥)
C. −sin 𝑥 cos (cos 𝑥)
D. sin 𝑥 cos (sin 𝑥)
3. If f is differentiable on the closed interval [a, b] and r is any number between f ’ (a) and
f ’ (b), then there exists a number c in the open interval (a, b) such that f ’(c) = r. This
statement is of
A. intermediate value theorem
B. mean value theorem
C. Rolle’s theorem
D. Darboux’s theorem
−1 𝑥
𝑒 𝑠𝑖𝑛ℎ
4. is the derivative of the function
√1+𝑥 2
−1
𝑒 𝑠𝑖𝑛ℎ 𝑥
A. x
√1+𝑥 2
−1 𝑥
𝑒 𝑠𝑖𝑛ℎ
B.
√1+𝑥 2
𝑠𝑖𝑛ℎ−1 𝑥
C. 𝑒 ans
−1 𝑥
D. 𝑒 𝑐𝑜𝑠ℎ
𝑑 𝑠𝑖𝑛𝑥
6. 𝑒 =
𝑑𝑥
A. 𝑒 𝑠𝑖𝑛𝑥 cos 𝑥
B. cos (sin 𝑥)
C. − 𝑒 𝑠𝑖𝑛𝑥 cos 𝑥
D. sin 𝑥 cos (sin 𝑥)
𝒔𝒊𝒏𝒙
9. Let 𝒇(𝒙) = . The first derivative of 𝒇(𝒙) at 𝒙 = 𝟎 is given by
𝟏+𝒙𝟐
A. 1
B. 0
C. -1
D. 2
11. For 𝑦 = 𝑡𝑎𝑛−1 𝑥, (1 + 𝑥 2 )𝑦𝑛+2 + 2(𝑛 + 1)𝑥𝑦𝑛+1 + 𝑛(𝑛 + 1)𝑦𝑛 = 0, Then 𝑦3 (0) is
A. 0
B. 1
C. 2
D. -2
𝑑
12. 𝑒 −𝑠𝑖𝑛𝑥 =
𝑑𝑥
A. −𝑒 −𝑠𝑖𝑛𝑥 cos 𝑥
B. cos (sin 𝑥)
C. − 𝑒 𝑠𝑖𝑛𝑥 cos 𝑥
D. sin 𝑥 cos (sin 𝑥)
6. A 7. D 8. A 9. A 10. C
11. D 12. A
Review Questions
1. Find the first three derivatives of the following expressions w.r.t. x
𝑥 2 +𝑎
(i)
𝑥+𝑎
2
(ii) 8𝑥 + 3.8𝑥 3 − 𝑥 2 + 𝑥 − 7
4
3
𝑠 = 12 − 4.5𝑡 + 6.2𝑡 2
find its velocity and acceleration when t=4 seconds, 𝑠 being in feet. Is the acceleration the
same for all values of 𝑡?
Further Reading
George B. Thomas Jr., Joel Hass, Christopher Heil& Maurice D. Weir (2018). Thomas’
Calculus (14th edition). Pearson Education.
Howard Anton, I. Bivens& Stephan Davis (2016).Calculus (10th edition).Wiley India.
http://www.calculusmadeeasy.org/7.html
https://www.math24.net/leibniz-formula
Objectives
Students will be able to
expand the functions using Maclaurin’s theorem
expand the functions using Taylor’s theorem
apply the Taylor’s theorem in finite form with Lagrange form of remainder
apply the Taylor’s theorem in finite form with Cauchy form of remainder
Introduction
In calculus, Taylor's theorem gives us a polynomial which approximates the function in terms of
the derivatives of the function. Since the derivatives are usually easy to compute, these polynomials
are also easy to compute.
A simple example of Taylor's theorem is the approximation of the exponential function 𝑒 near
𝑥 = 0. In other words, the exponential function can be approximated by an infinite polynomial
given as follows
𝑥 𝑥 x
𝑒 = 1+𝑥+ + + ⋯+ +⋯
2! 3! 𝑛!
For a derivable function𝑓, we can say that 𝑓′ exists in certain neighborhood of point 𝑐 and this
further implies that 𝑓 is defined and is continuous in a neighborhood of 𝑐.
Similarly, if 𝑓′ has derivative at 𝑐 has the same meaning as 𝑓 has a second derivative at 𝑐. And this
further implies that 𝑓′ is continuous at 𝑐.
In general if 𝑓 (𝑥) exists in the neighborhood of 𝑐, then the derivative of 𝑓 (𝑥) at 𝑐, if exists, is
called the 𝑛 derivative of 𝑓 at 𝑐 and is written as 𝑓 ( ) (𝑐).
(𝑎 + ℎ − 𝑥)
𝜙 (𝑥) = 0 ⇒ 𝑓 (𝑥) = 𝑝𝐴(𝑎 + ℎ − 𝑥)
(𝑛 − 1)!
(𝑎 + ℎ − 𝑎 − 𝜃ℎ)
𝜙 (𝑎 + 𝜃ℎ) = 0 ⇒ 𝑓 (𝑎 + 𝜃ℎ) = 𝑝𝐴(𝑎 + ℎ − 𝑎 − 𝜃ℎ)
(𝑛 − 1)!
(ℎ − 𝜃ℎ)
⇒ 𝑓 (𝑎 + 𝜃ℎ) = 𝑝𝐴(ℎ − 𝜃ℎ)
(𝑛 − 1)!
(1 − 𝜃)ℎ
⇒ 𝐴= 𝑓 (𝑎 + 𝜃ℎ), 1 − 𝜃 ≠ 0, ℎ≠0
(𝑛 − 1)! 𝑝
Substituting 𝐴 in the expression (2), we get the required result.
Corollary
Let 𝑥 be a point of the interval [𝑎, 𝑎 + ℎ]. Let 𝑓 satisfies the conditions of Taylor’s theorem in
[𝑎, 𝑎 + ℎ], thus it satisfies the condition for [𝑎, 𝑥] also.
Writing 𝑎 + ℎ as 𝑥 or ℎ as 𝑥 − 𝑎 in the expression (1), we get
𝑓 (𝑎) 𝑓 (𝑎) 𝑓 (𝑎) (𝑥 − 𝑎) (1 − 𝜃)
𝑓(𝑥) = 𝑓(𝑎) + (𝑥 − 𝑎) + (𝑥 − 𝑎) + ⋯ + (𝑥 − 𝑎) + 𝑓 (𝑎 + 𝜃(𝑥
1! 2! 𝑛! (𝑛 − 1)! 𝑝
− 𝑎))
---- (3)
where0 < 𝜃 < 1 and the expression (3) holds for all 𝑥 ∈ [𝑎, 𝑎 + ℎ].
Show that
𝑥 𝑥 x 𝑥
𝑒 =1+𝑥+ + + ⋯+ + 𝑒
2! 3! (𝑛 − 1)! 𝑛!
Here𝑓(𝑥) = 𝑒
𝑓 (𝑥)is continuous in [0, ℎ]
𝑓 (𝑥)exists in (0, ℎ)
Let 𝑝 = 𝑛 in (4). Then,
𝑓 (𝑥)
(𝑥 = 𝑒 𝑓 (0) = 1
𝑓 (𝑥)
(𝑥 = 𝑒 𝑓 ′(0) = 1
𝑓 (𝑥)
(𝑥 = 𝑒 𝑓 (0) = 1
𝑓 (𝑥)
(𝑥 = 𝑒 𝑓 (0) = 1
𝑓 (𝑥)
( ) = 𝑒 𝑓 (𝜃𝑥) = 𝜃𝑥
Therefore, fromthe expression (4), we get
𝑥 𝑥 x 𝑥
𝑒 =1+𝑥+ + + ⋯+ + 𝑒
2! 3! (𝑛 − 1)! 𝑛!
Hence the proof.
The expression of 𝑓(𝑥) in (5) will fail for those values of 𝑥 for which
(i) or any of its differential coefficient becomes infinite.
𝑓(𝑥)or
(ii) 𝑓(𝑥) or any of its differential coefficients is discontinuous and
92
Similarly the expansion of 𝑓(𝑥) by Maclaurin’s theorem is not valid for the values of 𝑥 for which
(i) 𝑓(0) or any of 𝑓 (0), 𝑓 (0), … is not finite
(ii) 𝑓(𝑥) or any of its derivatives is discontinuous as 𝑥 passes through zero and
(iii) lim → 𝑅 ≠ 0 i.e. lim 𝑓 (𝜃𝑥) ≠ 0
→ !
is valid for all values of 𝑛 for which lim → 𝑅 = 0.. The expression (6) is called Maclaurin’s infinite
series for the expansion of 𝑓(𝑥) as power series.
And if 𝑥 < 0
Then – 𝑥 > 0
Therefore 𝜃 > 0
⇒ −𝜃𝑥 > 0
⇒𝑒 >𝑒
⇒𝑒 <1
Therefore 𝑅 → 0 as 𝑛 → ∞ ∀ 𝑥 ∈ 𝑹
93
LOVELY PROFESSIONAL UNIVERSITY
Notes
Unit 10: Maclaurin’s and Taylor’s Theorems
∀ 𝑥∈𝑹
𝑥 𝑥
𝑠𝑖𝑛𝑥 = 𝑥 − + −⋯
3! 5!
Let 𝑎 = ∀ 𝑥 ∈ 𝑹 𝑎𝑛𝑑 𝑛 ∈ 𝑵
!
If 𝑥 = 0 lim → 𝑎 =0
If 𝑥 > 0 then for ∈ 𝑵 , 𝑎 > 0
For sufficiently large 𝑛 (say 𝑛 ≥ 𝑥)
𝑥 𝑥
𝑎 = = 𝑎 <𝑎
((𝑛 + 1)! 𝑛 + 1
This implies that after certain 𝑛, 𝑎 <𝑎
Since a bounded monotonically decreasing sequence of real numbers must have a limit,
𝑎 = lim 𝑎 = lim 𝑎
→ →
𝑥
= lim lim 𝑎
→ 𝑛+1 →
⇒ 𝑎=0
Hence proved
Therefore the
he Taylor’s theorem with Cauchy
Cauchy’s form of remainder is given as,
𝑓 (𝑎) 𝑓 (𝑎)
( ) 𝑓 (𝑎) ℎ (1 − 𝜃)
𝑓(𝑎 + ℎ) = 𝑓(𝑎) + ℎ +ℎ +⋯+ℎ + 𝑓 (𝑎 + 𝜃ℎ)
1! 2! (𝑛 − 1)! (𝑛 − 1)!!
or
( ) ( ) ( ) ( ) ( )
𝑓(𝑥) = 𝑓(𝑎) + (𝑥 − 𝑎) + (𝑥 − 𝑎) + ⋯ + (𝑥 − 𝑎) ( )!
+ ( )!!
𝑓 (𝑎 + 𝜃(𝑥 −
! !
𝑎)) ----- (6)
94
Now −1 < 𝑥
⇒ −𝜃 < 𝜃𝑥
⇒ 1 − 𝜃 < 1 + 𝜃𝑥
1−𝜃
⇒ <1
1 + 𝜃𝑥
1−𝜃
⇒0< <1
1 + 𝜃𝑥
Let 𝑚 − 1 > 0, we have
0<𝜃<1
⇒ 𝜃𝑥 < 𝑥
⇒ 𝜃𝑥 + 1 < 𝑥 + 1
⇒ 𝜃𝑥 + 1 < 2
Therefore
0 < 𝜃𝑥 + 1 < 2
⇒ 0 < (𝜃𝑥 + 1) <2 <2
⇒ (𝜃𝑥 + 1) ≤ (1 − |𝑥|)
( )…( )
We know, lim → ( )!
=0
∴ 𝑅 → 0 as 𝑛 → ∞ if|𝑥| < 1
( )
∴ (1 + 𝑥) = 1 + 𝑚𝑥 + !
𝑥 + ⋯when−1 < 𝑥 < 1
Expansion of 𝒍𝒐𝒈(𝟏 + 𝒙)
(1 + 𝑥) possesses continuous derivatives of every order when 1 + 𝑥 > 0 i.e. 𝑥 > −1. Also
(−1) (𝑛 − 1)!
𝑓 (𝑥) =
(1 + 𝑥)
Taking Cauchy’s form of remainder
⇒−θ< 𝜃𝑥 <𝜃
⇒1 −θ < 1+ 𝜃 𝑥 < 1 + 𝜃
1−θ
⇒0 < <1
1 + θx
1−θ
⇒ <1
1 + θx
Also we have
𝜃𝑥 > −|𝑥|
⇒ 1 + 𝜃𝑥 > 1 − |𝑥|
1 1
⇒ <
1 + 𝜃𝑥 1 − |𝑥|
Therefore, for all 𝑛
1
|𝑅 | < |𝑥| → 0 as 𝑛 → ∞
1 − |𝑥|
Therefore, when |𝑥| < 1,
𝑥 𝑥 (−1) 𝑥
log(1 + 𝑥) = 𝑥 − + − ⋯+ +⋯
2 3 𝑛−1
By taking the Lagrange’s form of remainder we may show that the infinite series expansion is valid
for 𝑥 = 1 also.
For the formal expansion of a function, we will follow the following steps:
97
LOVELY PROFESSIONAL UNIVERSITY
Notes
Unit 10: Maclaurin’s and Taylor’s Theorems
𝑒 𝑦 +𝑒 𝑦 =𝑒 ---- (3)
Differentiating again both sides w.r.t.𝑥
𝑒 𝑦 + 3𝑦 𝑦 𝑒 + 𝑒 𝑦 = 𝑒 ---- (4)
Differentiating again both sides w.r.t.𝑥
𝑒 𝑦 + 𝑦 𝑒 𝑦 + 3 𝑦 𝑦 𝑒 𝑦 + 𝑒 (𝑦 𝑦 + 𝑦 ) + 𝑒 3𝑦 𝑦 + 𝑦 𝑒 𝑦 = 𝑒 ---- (5)
(3) ⇒ 𝑒 𝑦 +𝑒 =1
1
(𝑦 ) =
4
(4) ⇒ 2𝑦 + 3 2+2 =1
3 1
2𝑦 + + = 1
4 4
(𝑦 ) = 0
(5) ⇒ (𝑦 ) = −
∴ By Maclaurin
Maclaurin's theorem
𝑥
𝑦 = (𝑦) + 𝑥 (𝑦 ) + (𝑦 ) + ⋯
2!
1 1 1
log(1 + 𝑒 ) = 𝑙𝑜𝑔2
𝑙𝑜𝑔 + 𝑥 + 𝑥 − 𝑥 +⋯
2 8 192
Let 𝑓(𝑥) = 𝑒 ,𝑥 ≠ 0
Let us look into the differentiability of the function at 𝑥 = 0
𝑓(0 + ℎ) − 𝑓(0)
lim 𝑓 ((0)) = lim
→ → ℎ
𝑒
= lim
→ ℎ
Substituting = 𝜃, we can write
𝑒
lim 𝑓 (0) = lim
→ → 1/𝜃
𝜃
= lim
𝑒 →
1
= lim =0
→ 2𝜃𝑒
𝑓(0 − ℎ) − 𝑓(0)
lim 𝑓 ((0)) = lim
→ → −ℎ
𝑒
= lim =0
→ −ℎ
∴ 𝑓 (0) = 0
Also, 𝑓 (𝑥) = 𝑒 ,𝑥 ≠ 0
2
lim 𝑓 (𝑥) = lim 𝑒
→ → 𝑥
Substituting = 𝑡
98
LOVELY PROFESSIONAL UNIVERSITY
Notes
Calculus
2𝑡
lim 𝑓 (𝑥) = lim = 0 = 𝑓′(0)
→ → 𝑒
Therefore the function is continuous at 𝑥 = 0.
If we find the higher derivative of 𝑓(𝑥)for 𝑥 ≠ 0, we will get 𝑒 multiplied by a
polynomial in .
Therefore, higher derivatives of 𝑓(𝑥)will be zero at 𝑥 = 0.
So, the function possesses continuous derivatives for every value of 𝑥.
By Maclaurin’s theorem
𝑥 𝑥
𝑓(𝑥) = 𝑓(0) + 𝑥𝑓 (0) + 𝑓 (0) + ⋯ + 𝑓 (0) + 𝑅
2! (𝑛 − 1)!
𝑥 𝑥
and so𝑒 = 0 + 𝑥. 0 + . 0 + ⋯ .0 + 𝑅
2! (𝑛 − 1)!
i.e.𝑅 = 𝑒
𝑅 does not approach to zero as 𝑛 approaches to infinity.
Therefore, 𝑓(𝑥) can not be expanded by Maclaurin’s theorem
Summary
In this unit, we learnt about the finite form of Taylor’s and Maclaurin’s theorem.
The Taylor’s theorem states that, if a function 𝑓 is such that
(i) the (𝑛 − 1) derivative 𝑓 is continuous in [𝑎, 𝑎 + ℎ],
(ii) the 𝑛 derivative 𝑓 exists in (𝑎, 𝑎 + ℎ) and
(iii) 𝑝 is a given positive integer
Then there exists at least one 𝜃 ∈ (0,1) such that
𝑓 (𝑎) 𝑓 (𝑎) 𝑓 (𝑎)
𝑓(𝑥) = 𝑓(𝑎) + (𝑥 − 𝑎) + (𝑥 − 𝑎) + ⋯ + (𝑥 − 𝑎)
1! 2! 𝑛!
(𝑥 − 𝑎) (1 − 𝜃)
+ 𝑓 (𝑎 + 𝜃(𝑥 − 𝑎))
(𝑛 − 1)! 𝑝
The Taylor’s theorem with Lagrange’s form of remainder is given as,
𝑓 (𝑎) 𝑓 (𝑎) 𝑓 (𝑎) ℎ
𝑓(𝑎 + ℎ) = 𝑓(𝑎) + ℎ +ℎ +⋯+ℎ + 𝑓 (𝑎 + 𝜃ℎ)
1! 2! (𝑛 − 1)! 𝑛!
The Taylor’s theorem with Cauchy’s form of remainder is given as,
𝑓 (𝑎) 𝑓 (𝑎) 𝑓 (𝑎) ℎ (1 − 𝜃)
𝑓(𝑎 + ℎ) = 𝑓(𝑎) + ℎ +ℎ +⋯+ℎ + 𝑓 (𝑎 + 𝜃ℎ)
1! 2! (𝑛 − 1)! (𝑛 − 1)!!
For the Maclaurin’s theorem with Lagrange and Cauchy’s form of remainder,
substitute𝑎 = 0 and ℎ = 𝑥 in the above expressions.
Keywords
Taylor’s theorem, Maclaurin’s theorem, Lagrange’s form of remainder, Cauchy’s form of
remainder, Taylor’s series, Maclaurin’s series
Self Assessment
1. If a function 𝑓 is derivable then which of the following is true?
A. 𝑓 is defined
B. 𝑓 is defined and is continuous in a neighborhood of a point 𝑐
C. 𝑓 is defined and is uniformly continuous in a neighborhood of a point 𝑐
D. none of these
5. The expansion of 𝑒 is
A. 1 + + + +⋯
B. 1− + + +⋯
C. 1+ − + +⋯
D. 1 + + − +⋯
6. The (𝑛 + 1) term in the generalized mean value theorem or the Taylor theorem for the
function 𝑓(𝑎 + ℎ) is
( )
A. ( )!
𝑓 (𝑎 + 𝜃ℎ)
( )
B. ( )!
𝑓 (𝑎 + 𝜃ℎ)
( )
C. ( )!
𝑓 (𝑎 + 𝜃ℎ)
( )
D. ( )!
𝑓 (𝑎 − 𝜃ℎ)
( )
7. In the expression ( )!
𝑓 (𝑎 + 𝜃ℎ) which of the following is true for the 𝜃 value?
A. 𝜃 ∈ [0,1]
B. 𝜃 ∈ (0,1)
C. 𝜃 can take any value
D. 𝜃>0
( )
8. The expression ( )!
𝑓 (𝑎 + 𝜃ℎ) is known as
A. Remainder term
B. Remainder after n terms
C. Remainder after n+1 terms
D. Remainder after n-1 terms
( )
9. ( )!
𝑓 (𝑎 + 𝜃ℎ) is due to
A. Schlomilch
B. Lagrange
C. Schlomilch and Roche
D. Cauchy
11. The Taylor’s theorem with Lagrange’s form of remainder for a function 𝑓(𝑥) will fail for
those values of 𝑥 for which
I. 𝑓(𝑥) or any of its differential coefficients becomes infinite
II. 𝑓(𝑥) or any of its differential coefficients becomes discontinuous
III. The remainder term is non-zero as 𝑛 → ∞
( )
12. The expression ( )!
𝑓 (𝑎 + 𝜃ℎ) is known as
A. Remainder term
B. Remainder after n terms
C. Remainder after n+1 terms
D. Remainder after n-1 terms
( )
13. ( )!
𝑓 (𝑎 + 𝜃ℎ) is due to
A. Schlomilch
B. Lagrange
C. Schlomilch and Roche
D. Cauchy
1. B 2. A 3. D 4. D 5. D
6. C 7. B 8. B 9. C 10. B
Review Questions
1. Expand cos 𝑥 by Maclaurin’s series.
2. Expand log(1 + 𝑥) by Maclaurin’s theorem.
3. Expand log(𝑥 + 𝑎)in the powers of 𝑥 by Taylor’s theorem.
4. Expand log sin 𝑥 in powers of (𝑥 − 2).
5. Expand sin (𝑥 + ℎ) in powers of 𝑥 till the power of 𝑥 .
6. Expand tan 𝑥 in the powers of 𝑥 − .
7. Differentiate in the Taylor’s theorem with the Lagrange’s and Cauchy’s form of remainder.
8. Differentiate in the Maclaurin’s theorem with the Lagrange’s and Cauchy’s form of
remainder.
9. By Maclaurin’s theorem, find first three non vanishing terms in the expansion of .
10. Expand 𝑒 cos 𝑥 in the form of a power series.
Further Reading
W. Thomas Finny (1998). Calculus and Analytic Geometry, 66th Edition,
Publishers, Narsa, India.
R. K. Jain, and Iyengar, SRK. (2010). Advanced Engineering Mathematics, 3 rd
Edition Publishers, Narsa, India.
Widder, D.V. (2002). Advance Calculus 22nd Edition, Publishers, PHI, India.
Piskunov, N. (1996). Differential and Integral Calculus Vol I, & II, Publishers,
CBS, India.
Online link
https://openstax.org/books/calculus
https://openstax.org/books/calculus-volume-2/pages/6-3-taylor-and-
maclaurin-series
https://math.libretexts.org
https://math.libretexts.org/Bookshelves/Calculus/Book%3A_Calculus_(Ope
nStax)/10%3A_Power_Series/10.3%3A_Taylor_and_Maclaurin_Series
Objectives
Students will be able to
Introduction
In this unit, we will see one very interesting application of calculus, and it is called the maxima and
minima of a function. When one says, Mount Everest or Mariana Trench, what comes to your
mind? You think of a high point on the surface of Earth, and a low point on the surface of Earth. So
if you can draw the Earth's topography, the highest point will refer to a place which is a mountain,
and that gives you the idea of the maximum height for any object on the earth. Similarly, the
minimum height or you can say the maximum depth is at the Mariana Trench, so these ideas of
maximum and minimum are inherently there in our daily lives. We can see one more example to
understand the topic better.
The adjacent graph is about a cricket match between Australia and India. The blue one is
representing the run rate of India and the green one is representing the run rate of Australia, with
respect to the overs. By mathematical
modeling, we can write the run rate in
terms of overs, i.e. a function can be
framed or we can define some formula
in such a way that run rate, say ‘y’,
can be written in terms of ‘x’ where x
is the overs.
Here the graph is available, on the
basis of the data of the actual match.
In the first over the run rate for the
Australian team was two only. And in
the first over the run rate for Indian
𝑓(𝑐 + ℎ) − 𝑓(𝑐)
ℎ<0 ⇒ >0
ℎ
A function is said to be stationary for 𝑐 and 𝑓(𝑐) a stationary value of 𝑓if 𝑓 ′ (𝑐) = 0. The rate of
change of a function is zero at the stationary point.
Find the greatest and least value of the function 𝑓(𝑥) = 3𝑥 4 − 2𝑥 3 − 6𝑥 2 + 6𝑥 + 1 in [0,2].
𝑓 ′ (𝑥) = 12𝑥 3 − 6𝑥 2 − 12𝑥 + 6
= 6(𝑥 − 1)(𝑥 + 1)(2𝑥 − 1)
Now by the necessary condition for an extreme value, 𝑓 ′ (𝑥) must be zero. And this gives 𝑥 =
1
1, −1, . Since -1 is not in the domain of the function, this value can be ignored. The other two
2
numbers are the candidates to be the point of maximum or minimum value of the function.
𝑓(1) = 2
1 39
𝑓( ) = = 2.43
2 16
Moreover we must check the value of the function at the end points of the domain also.
𝑓(0) = 1
𝑓(2) = 21
Thus the function has its maximum value at 𝑥 = 2 and minimum value at 𝑥 = 0.
Steps to find the absolute maximum and minimum values of a continuous function f
on a closed interval:
1. Find all critical points of f in the given interval.
2. Evaluate f at the critical point(s) found in step 1, as well as at the two endpoints of the interval.
3. The point(s) of the largest value of f is the absolute maximum(s), the point(s) of the smallest
value is the absolute minimum(s).
Let us understand this by an example.
Examine the polynomial 𝑓(𝑥) = 10𝑥 6 − 24𝑥 5 + 15𝑥 4 − 40𝑥 3 + 108 for maximum and
minimum value
Here 𝑓 ′ (𝑥) = 60𝑥 2 (𝑥 2 + 1)(𝑥 − 2)
For maximum and minimum value 𝑓 ′ (𝑥) = 0 implies that 𝑥 = 0, 2 are the only real values.
Now 𝑥 < 0 ⇒ 𝑓 ′ (𝑥) < 0
Therefore 𝑓′(𝑥) does not change sign as 𝑥 passes through 0, so that 𝑓(0) is neither a maximum nor a
minimum value and 𝑓′(𝑥) changes the sign from negative to positive as 𝑥 passes through 2.
∴ 𝑓(2) = −100is the minimum value.
∴ 𝑓(𝑥)has only one extreme value i.e. at 2.
Find all local maximum and minimum points for the function
𝑓(𝑥) = 𝑥 3 − 𝑥
The derivative is𝑓 ′ (𝑥) = 3𝑥 2 − 1.
1
This is defined everywhere and is zero at 𝑥 = ± .
√3
1 1 2√3
Looking first at 𝑥 =
√3
. we see that 𝑓 ( ) = −
√3 9
.
1
Now we test two points on either side of 𝑥 = , making sure that neither is farther away than the
√3
1
nearest critical value; since √3 < 3, < 1 and we can use 𝑥 = 0 and 𝑥 = 1 .
√3
2√3 2√3 1
Since 𝑓(0) = 0 > − and𝑓(1) = 0 > − , there must be a local minimum at𝑥 = .
9 9 √3
1 1 2√3
For𝑥 = − ., we see that(− )= .
√3 √3 9
This example is made very simple by our choice of points to test, for other choice of points the
calculations would have been comparatively lengthy.
Also, 𝑓 ′ (𝑐) = 0
∴ 𝑓 ′ (𝑥) < 0 ∀ 𝑥 ∈ [𝑐 − 𝛿, 𝑐) (strictly decreasing function)
and 𝑓 ′ (𝑥) > 0 ∀ 𝑥 ∈ [𝑐, 𝑐 + 𝛿) (strictly increasing function)
Theorem: 𝑓(𝑐) is a maximum value of the function 𝑓 if 𝑓 ′ (𝑐) = 0 and𝑓 ′′ (𝑐) < 0.
Proof: 𝑓 ′′ (𝑐) < 0 ⇒ ∃ an open interval(𝑐 − 𝛿, 𝑐 + 𝛿) around 𝑐 for every point 𝑥 of which, the second
derivative is negative.
⇒ 𝑓 ′ (𝑥)is strictly decreasing in (𝑐 − 𝛿, 𝑐 + 𝛿).
Also, 𝑓 ′ (𝑐) = 0
∴ 𝑓 ′ (𝑥) > 0 ∀ 𝑥 ∈ [𝑐 − 𝛿, 𝑐)(strictlyincreasing function)
and 𝑓 ′ (𝑥) < 0 ∀ 𝑥 ∈ [𝑐, 𝑐 + 𝛿) (strictly decreasing function)
So, from now onwards we can follow the following steps to find the maximum / minimum of a
function:
1 𝑥 1
Show that the maximum value of ( ) is 𝑒 𝑒 .
𝑥
1 𝑥
Let 𝑦 = ( )
𝑥
log 𝑦 = −𝑥 𝑙𝑜𝑔𝑥
Differentiating both sides w.r.t.𝑥.
𝑑𝑦 1 𝑥
= −(1 + log 𝑥) ( )
𝑑𝑥 𝑥
Applying the necessary condition for extreme values, we get
log 𝑥 = −1
𝑥 = 𝑒 −1
Now by the sufficient condition, we can check if the point 𝑥 = 𝑒 −1 is the point of maximum or a
point of minimum or neither of them.
1
𝑑2𝑦
At = 𝑒 −1 , = −𝑒. 𝑒 𝑒 < 0
𝑑𝑥 2
1
Therefore 𝑦 has a maximum for 𝑥 = 𝑒 −1 and the maximum value is 𝑒 𝑒 .
Find the maximum and minimum value of the function𝑓(𝑥) = 8𝑥 5 − 15𝑥 4 + 10𝑥 2.
The given function is 𝑓(𝑥) = 8𝑥 5 − 15𝑥 4 + 10𝑥 2
𝑓 ′ (𝑥) = 40𝑥 4 − 60𝑥 3 + 20𝑥
= 20𝑥(2𝑥 3 − 3𝑥 2 + 1)
= 20𝑥(𝑥 − 1)2 (2𝑥 + 1)
Putting 𝑓 ′ (𝑥) = 0 for the critical points, we get
1
𝑥 = 0, 1, −
2
Now these three points are the candidates to be the point of maximum or minimum or neither of
them. Let’s check with the help of the second derivative test.
We have
𝑓 ′′ (𝑥) = 160𝑥 3 − 180𝑥 2 + 20
𝑓 ′′ (𝑥)(𝑎𝑡 𝑥 = 0) = 20 > 0 ⇒ 𝑥 = 0 is a point of minimum
Find the absolute maximum and minimum points of f (x) = 4 − x2 on each of the intervals (i)
[−3, 1] and (ii) [2, 5].
Summary
In this unit we have seen how to calculate the maximum and minimum of a function if they exist.
• A function f has an absolute maximum (also called global maximum) at c if f (c) ≥ f (x) for
all x in its domain.
• A function f has an absolute minimum (or global minimum) at c if f (c) ≤ f (x) for all x in its
domain.
• The maximum and minimum values of f are called the extreme values of f.
• If f is continuous on a closed interval [a, b] , then there exist (at least) a point c where f
attains its maximum value, f (c), on the interval, and (at least) a point d where f attains its
minimum value, f (d), on the interval.
• 𝑓(𝑐) is an extreme value of 𝑓 if and only if 𝑓′(𝑥) changes sign as 𝑥 passes through 𝑐.
• 𝑓(𝑐)is a minimum value of the function 𝑓 if 𝑓 ′ (𝑐) = 0 and𝑓 ′′ (𝑐) > 0.
• 𝑓(𝑐)is a maximum value of the function 𝑓 if 𝑓 ′ (𝑐) = 0 and𝑓 ′′ (𝑐) < 0.
Key Words
Maxima, Minima, maximum of a function, minimum of a function, First derivative test, critical
points, stationary points, second derivative test, Extreme value theorem, Fermat’s theorem
Self Assessment
1. What is the saddle point?
A. Point where function has maximum value
B. Point where function has minimum value
C. Point where function has zero value
D. Point where function neither has maximum value nor minimum value
4. Find the maximum and minimum of 𝑓(𝑥) = 𝑥 3 − 6𝑥 2 + 9𝑥 + 1 on the interval [0, 5].
A. 𝑓 ′ (𝑐) ≠ 0
B. 𝑓(𝑐) = 0
C. 𝑓 ′ (𝑐) = 0
D. 𝑓 ′′ (𝑐) = 0
A. 2
B. √2
C. 1
D. 1 + √2
1
7. The maximum value of 𝑓(𝑥) = 𝑥 3 − 2𝑥 2 + 3𝑥 + 1 is
3
A. 3/7
B. 7/3
C. 1
D. 7
D. none of these
11. The saddle points for the function 10𝑥 6 − 24𝑥 5 + 15𝑥 4 − 40𝑥 3 + 108 are
A. 0, 1, 2
B. -1, 0, 2
C. 1, 2
D. 0, 2
A. -1/2, 0
B. 0, 1, ½
C. -1/2, 0, 1
D. none of these
A. a point of minimum
B. a point of maximum
C. point of inflexion
D. none of these
1
14. For the function8𝑥 5 − 15 𝑥 4 + 10 𝑥 2, 𝑥 = − is
2
A. a point of minimum
B. a point of maximum
C. point of inflexion
D. none of these
A. a point of minimum
B. a point of maximum
C. point of inflexion
D. neither a point of maximum nor a point of minimum
6. B 7. B 8. A 9. B 10. B
Further Reading
W. Thomas Finny (1998). Calculus and Analytic Geometry, 6th Edition, Publishers, Narsa,
India.
R. K. Jain, and Iyengar, SRK. (2010). Advanced Engineering Mathematics, 3 rd Edition
Publishers, Narsa, India.
Widder, D.V. (2002). Advance Calculus 2nd Edition, Publishers, PHI, India.
Piskunov, N. (1996). Differential and Integral Calculus Vol I, & II, Publishers, CBS, India.
https://opentextbc.ca/calculusv1openstax/chapter/maxima-and-minima/
https://www.mathsisfun.com/calculus/maxima-minima.html
https://www.whitman.edu/mathematics/calculus_online/section05.01.html
Objectives
Students will be able to
Introduction
This unit is about two important
applications of derivatives namely
curvature and the asymptotes. Consider
that you are having a road trip in a hilly
region. Imagine the roads. You have the
technique to measure the distance
between any two points on a straight line.
But how to measure the bend happening
at a particular point needs some
elaboration on curvature! Similarly
another crucial feature of differential
calculus is the concept of asymptotes.
Basically it provides a frame for any curve
12.1 Curvature
Curvature is the numerical measure of bending of a curve. At a particular point on the curve, a
tangent can be drawn. Let this line makes an angle 𝜓 with positive x- axis. Then curvature is
defined as the magnitude of rate of change of 𝜓with respect to the arc length 𝑠.
It is quite intuitive that the smaller circle bends more sharply than larger circle and thus smaller
circle has a larger curvature and larger the circle, smaller will be its curvature.
Let us consider a circle with center 𝑂 and radius 𝑟. Let the arc𝑃𝑄 = Δ𝑠
Arc 𝑃𝑄
Angle 𝑃𝑂𝑄 =
𝑂𝑃
Δ𝜓 1
=
Δ𝑠 𝑟
Δ𝜓 𝑑𝜓 1
lim = =
𝑄→𝑃 Δ𝑠 𝑑𝑠 𝑟
Therefore, curvature at any point of a circle is the reciprocalof the radius, and hence is a constant.
Find the radius of curvature at any point for the curve 𝑠 = 𝑐 tan 𝜓
We have
𝑑𝑠
𝜌=
𝑑𝜓
∴ 𝜌 = 𝑐 sec 2 𝜓
Find the radius of curvature at any point for the curve 𝑠 = 𝑐 log sec 𝜓
We have
𝑑𝑠
𝜌=
𝑑𝜓
∴ 𝜌 = 𝑐 𝑡𝑎𝑛 𝜓
chord𝑃𝑄 2 Δ𝑠 2 Δ𝑦 2
( ) ( ) = 1+( )
𝑎rc𝑃𝑄 Δ𝑥 Δ𝑥
As 𝑄 → 𝑃, the chord 𝑃𝑄 and arc 𝑃𝑄 become almost same making the above expression as
d𝑠 2 d𝑦 2
( ) =1+( )
d𝑥 d𝑥
d𝑠 d𝑦 2
= √1 + ( )
d𝑥 d𝑥
d𝑠 2 d𝑥 2 d𝑦 2
( ) =( ) +( )
d𝑡 d𝑡 d𝑡
12.4 Radius of Curvature- Cartesian Equations
Consider a curve 𝑦 = 𝑓(𝑥)
𝑑𝑦
We have tan 𝜓 =
𝑑𝑥
3𝑎 3𝑎 8√2
Show that the curvature of the point ( , ) on the Folium 𝑥 3 + 𝑦 3 = 3𝑎𝑥𝑦is − .
2 2 3𝑎
And
𝑑2 𝑦 32
( 2) =−
𝑑𝑥 3𝑎,3𝑎 3𝑎
2 2
3𝑎 3𝑎
Therefore the curvature at the point ( , ) is
2 2
3
𝑑𝑥 2 2
1 [1 + ( ) ]
𝑑𝑦
= 𝑑2𝑥
𝜌
𝑑𝑦 2
8√2
= −
3𝑎
𝑡
For the cycloid 𝑥 = 𝑎(𝑡 + 𝑠𝑖𝑛𝑡), 𝑦 = 𝑎(1 − cos 𝑡), prove that 𝜌 = 4 a cos .
2
𝑑𝑥
= 𝑎(1 + cos 𝑡)
𝑑𝑡
𝑑𝑦
= 𝑎 sin 𝑡
𝑑𝑡
𝑑𝑦 𝑡
= tan
𝑑𝑥 2
𝑑2 𝑦 1 𝑡 𝑑𝑡
= sec 2
𝑑𝑥 2 2 2 𝑑𝑥
1 1
=
4𝑎 cos4 𝑡
2
3
𝑑𝑥 2 2
[1+( ) ] 𝑡
𝑑𝑦
The radius of curvature 𝜌 = 𝑑2 𝑥
= 4𝑎 cos .
2
𝑑𝑦2
𝑑𝑦 𝑟1 sin 𝜃 + 𝑟 cos 𝜃
∴ 𝑦1 = =
𝑑𝑥 𝑟1 𝑐𝑜𝑠𝜃 − 𝑟 sin 𝜃
3
𝑑2 𝑦 (𝑟 2 + 𝑟12 )2
𝑦2 = 2 =
𝑑𝑥 (𝑟1 𝑐𝑜𝑠𝜃 − 𝑟𝑠𝑖𝑛𝜃)3
where𝑟1 = 𝑓 ′ (𝜃), 𝑟2 = 𝑓′′(𝜃)
Thus the radius of curvature can be written as
3
(𝑟 2 + 𝑟12 )2
𝜌=
𝑟 2 + 2𝑟12 − 𝑟 𝑟2
𝑎𝑚
For the curve 𝑟 𝑚 = 𝑎𝑚 cos 𝑚𝜃, prove that 𝜌 = (𝑚+1)𝑟 𝑚−1.
Taking logarithm on both sides of the given equation and then differentiating w.r.t. 𝜃, we get
𝑚 𝑑𝑟 𝑠𝑖𝑛 𝑚𝜃
= −𝑚
𝑟 𝑑𝜃 𝑐𝑜𝑠𝑚𝜃
𝑟1 = −𝑟 tan 𝑚𝜃
𝑑2 𝑟
𝑟2 = = −𝑟𝑚 𝑠𝑒𝑐 2 𝑚𝜃 + 𝑟 tan2 𝑚𝜃
𝑑𝜃 2
Using
3
(𝑟 2 + 𝑟12 )2
𝜌=
𝑟 2 + 2𝑟12 − 𝑟 𝑟2
We get
𝜌 = (𝑟 3 sec 3 𝑚𝜃) /(𝑟 2 sec 2 𝑚𝜃 + 𝑚𝑟 2 sec 2 𝑚𝜃)
1 𝑎𝑚
𝜌=
𝑚 + 1 𝑟 𝑚−1
𝐥𝐢𝐦 𝒚 − 𝒎𝒙 = 𝒄
𝒙→∞
𝑦 1
Also − 𝑚 = (𝑦 − 𝑚𝑥)
𝑥 𝑥
𝑦 1
lim ( − 𝑚) = lim (𝑦 − 𝑚𝑥). lim = 0
𝑥→∞ 𝑥 𝑥→∞ 𝑥→∞ 𝑥
This implies
𝒚
𝐥𝐢𝐦 =𝒎
𝒙→∞ 𝒙
Put 𝑦 + 𝑥 = 𝑝
As 𝑥 → ∞, 𝑝 → 𝑐
Put 𝑦 = 𝑝 − 𝑥 in (1)
𝑥 3 + (𝑝 − 𝑥)3 − 3𝑎𝑥(𝑝 − 𝑥) = 0
1 𝑝3
3(𝑝 + 𝑎) − 3𝑝(𝑝 + 𝑎) + 2 = 0
𝑥 𝑥
As 𝑥 → ∞, 𝑝 → 𝑐
3(𝑐 + 𝑎) = 0
𝑐 = −𝑎
∴ The equation of the asymptote is 𝑦 = −𝑥 − 𝑎.
For a general formula we arrange the given curve in descending powers of 𝑦 i.e.
𝑦 𝑚 𝜙(𝑥) + 𝑦 𝑚−1 𝜙1 (𝑥) + 𝑦 𝑚−2 𝜙2 (𝑥) + ⋯ = 0 ---- (2)
where𝜙(𝑥), 𝜙1 (𝑥), 𝜙2 (𝑥) … are the polynomials in 𝑥.
Dividing (2) by 𝑦 𝑚 , we get
1 1
𝜙(𝑥) + 𝜙1 (𝑥) + 𝜙2 (𝑥) + ⋯ = 0 ---- (3)
𝑦 𝑦2
Let 𝑦 → ∞
then lim 𝑥 = 𝑘
𝑦→∞
𝜙(𝑘) = 0
Therefore 𝑘 is the root of equation 𝜙(𝑥) = 0. Let 𝑘1 , 𝑘2 etc. be the roots of 𝜙(𝑥) = 0, then the
asymptote parallel to y-axis are 𝑥 = 𝑘1 , 𝑥 = 𝑘2 etc.
⇒ (𝑥 − 𝑘1 )(𝑥 − 𝑘2 )etc. are the factors of 𝜙(𝑥) which is the coefficient of highest power 𝑦 𝑚 of y in the
given equation.
Similarly the derivation can be done for the asymptotes parallel to the x axis and can be
summarized as the following rules:
Rule 1: The asymptotes parallel to Y axis are obtained by equating to zero, the real linear factors in
the coefficient of highest power of y, in the equation of the curve.
Rule 2: The asymptotes parallel to X axis are obtained by equating to zero, the real linear factors in
the coefficient of highest power of x, in the equation of the curve.
Find the asymptote parallel to the coordinate axes of the curve
(𝑥 2 + 𝑦 2 )𝑥 − 𝑎𝑦 2 = 0
The equation can be re written as
𝑥 3 + 𝑦 2 (𝑥 − 𝑎) = 0
Coefficient of highest power of 𝑥 is 1 and that cannot be equated to zero. Therefore the asymptote
parallel to the x-axis does not exist.
Coefficient of highest power of 𝑦 is 𝑥 − 𝑎 and equating it to zero gives 𝑥 − 𝑎 = 0.Therefore the
asymptote parallel to the y-axis is 𝑥 = 𝑎.
Dividing by 𝑥 𝑛
𝑦 1 𝑦 1 𝑦 1 𝑦
𝜙𝑛 ( ) + 𝜙𝑛−1 ( ) + ⋯ + 𝑛−1 𝜙1 ( ) + 𝑛 𝜙0 ( ) = 0
𝑥 𝑥 𝑥 𝑥 𝑥 𝑥 𝑥
and taking the limit 𝑥 → ∞, we get
Expanding each term by Taylor’s theorem and re arranging the terms, we get
𝑝12 ′′ ′
𝑥 𝑛 𝜙𝑛 (𝑚1 ) + 𝑥 𝑛−1 (𝑝1 𝜙𝑛′ (𝑚1 ) + 𝜙𝑛−1 (𝑚1 )) + 𝑥 𝑛−2 ( 𝜙 (𝑚 ) + 𝑝1 𝜙𝑛−1 (𝑚1 ) + 𝜙𝑛−2 (𝑚1 )) + ⋯ = 0
2 𝑛 1
1 𝑝12 ′
(𝑝1 𝜙𝑛′ (𝑚1 ) + 𝜙𝑛−1 (𝑚1 )) + ( 𝜙𝑛′′ (𝑚1 ) + 𝑝1 𝜙𝑛−1 (𝑚1 ) + 𝜙𝑛−2 (𝑚1 )) + ⋯ = 0
𝑥 2
𝜙𝑛−1 (𝑚1 )
Therefore 𝑦 = 𝑚1 𝑥 − ′ (𝑚 ) is the asymptote corresponding to slope𝑚1 .
𝜙𝑛 1
(𝑚2 − 1)(𝑚 − 1) = 0
𝑚 = 1, 1, −1
𝜙 (𝑚)
When 𝑚 = 1, 𝑐 = − 2′ (𝑚)
𝜙3
Summary
• The total bending or total curvature is Arc𝑃𝑄 or Angle Δ𝜓
Δ𝜓
• The average curvature is
Δ𝑠
Δ𝜓 d𝜓
• The curvature of the curve at P is lim =
𝑄→𝑃 Δ𝑠 d𝑠
3
𝑑𝑥 2 2
[1+( ) ]
•
𝑑𝑦
Radius of curvature for a Cartesian curve 𝜌 = 𝑑2 𝑥
𝑑𝑦2
3
(𝑓′2 (𝑡)+𝑔′2 (𝑡))2
• Radius of curvature for a parametric curve 𝜌 =
𝑓′ (𝑡)𝑔′′ (𝑡)−𝑔′ (𝑡)𝑓′′ (𝑡)
3
(𝑟 2 +𝑟12)2
• Radius of curvature for a polar curve 𝜌 = 2 2
𝑟 +2𝑟1 −𝑟 𝑟2
• The asymptotes parallel to Y axis are obtained by equating to zero, the real linear factors in
the coefficient of highest power of y, in the equation of the curve.
Key Words
Curvature, radius of curvature, vertical asymptote, horizontal asymptote, oblique asymptotes
Self Assessment
1. The angle through which the tangent turns as a point moves along the curve from a point
P to Q, will be large or small as compared to arc length, depends upon
A. slope of tangent
B. sharpness of bend
C. velocity
D. acceleration
3. The reciprocal of the curvature of a curve at any point in case it is non- zero, is called
A. curvature
B. radius of curvature
C. bend
D. total bending
6. For the cycloid 𝑥 = 𝑎(𝑡 + 𝑠𝑖𝑛 𝑡), 𝑦 = 𝑎(1 − 𝑐𝑜𝑠 𝑡), the radius of curvature is given as
A. 4𝑎 cos 𝑡
𝑡
B. 4 cos
2
6. D 7. C 8. B 9. A 10. D
Review Questions
1. If the radius of circle A is 1/6, then its curvature is ____________.
B
A
Further Reading
W. Thomas Finny (1998). Calculus and Analytic Geometry, 6th Edition, Publishers, Narsa,
India.
R. K. Jain, and Iyengar, SRK. (2010). Advanced Engineering Mathematics, 3 rd Edition
Publishers, Narsa, India.
Widder, D.V. (2002). Advance Calculus 2nd Edition, Publishers, PHI, India.
Piskunov, N. (1996). Differential and Integral Calculus Vol I, & II, Publishers, CBS, India.
https://www.whitman.edu/mathematics/calculus_online/section13.03.html
https://www.math24.net/curvature-plane-curves
https://www.semanticscholar.org/paper/Asymptotes%2C-Cubic-Curves%2C-and-the-
Projective-Plane-Nunemacher/82e455119d0ad5d7ad8c56770792302ed4c89263?p2df
https://www.intmath.com/applications-differentiation/8-radius-curvature.php
Objectives
Students will be able to
Introduction
In this unit, we will mainly learn about various important aspects involved in the tracing of a curve.
We will begin with the symmetry and its various aspects in relation to different shapes. From the
differentiability we have the idea of smoothness or pointedness of the curve at a point. This idea
can be extended to concavity of a function, with a special focus on the points of inflection. There
will be further a discussion on the types of double points, their nature and their position.
13.1 Symmetry
The images which can be divided into identical halves are called symmetrical. The images that
cannot be divided into identical halves are asymmetrical.
Any line splitting a shape into two parts such that the two parts are the same is called a line of
symmetry. These parts are also said to be symmetrical to each other.
For a square there are four lines of symmetry. for a hexagon, there will be six lines of symmetry.
Can you think of the lines of symmetry for a triangle and a pentagon?
You can take a piece of paper, draw the required shape on it, using the scale and pencil, cut out
them and fold it in various ways to find out the lines of symmetry.
Consider the folium of Descartes and the cardioid; you can observe that there is only one line of
symmetry.
(i) 𝑦 2 (2𝑎 − 𝑥) = 𝑥 3
(ii) (𝑥 2 + 𝑦 2 )2 = 𝑎2 (𝑥 2 − 𝑦 2 )
(iii) (𝑥 − 𝑏)2 (𝑥 2 + 𝑦 2 ) − 𝑎2 𝑥 2 = 0
(iv) 𝑥 3 + 𝑦 3 = 3𝑎𝑥𝑦
(v) (𝑥 2 + 𝑦 2 − 𝑎𝑥𝑦)2 = 4𝑎2 (𝑥 2 + 𝑦 2 )
(vi) 𝑥 2 + 𝑦 2 = 16
(vii) 𝑦 2 = 2𝑥
(viii) 𝑥 2 + 𝑦 = 2𝑥 + 4
Theorem:
Consider a function f(x) that is twice continuously differentiable on an interval I. The
Function f(x) is
2
𝑓 ′′ (𝑥) > 0 in (− , ∞) ⇒ 𝑓(𝑥) is concave upward in this interval.
15
5
Find the point of inflection for the curve 𝑓(𝑥) = 𝑥 + 𝑥 3
Finding the derivatives, we get
5 2
𝑓 ′ (𝑥) = 1 + 𝑥 3
3
10
𝑓 ′′ (𝑥) = 1
9𝑥 3
Here the 𝑓 ′′ (𝑥) = 0 won’t make sense, so using the first derivative test, we can observe that
when𝑥 < 0, 𝑓 ′′ (𝑥) < 0 and when 𝑥 > 0, 𝑓 ′′ (𝑥) > 0.
So we can see the curve changes from concave downward to concave upward at (0, 0), So (0, 0) is
the point of inflection of the given curve.
Then when 𝑥 → 0, 𝑦 → 0
𝑦
lim = 𝑚is the slope of the tangent.
𝑥
So (1) implies
𝑦 𝑦 𝑦
(𝑏1 + 𝑏2 ) + (𝑐1 𝑥 + 𝑐2 + 𝑐3 𝑦 ) + ⋯ = 0
𝑥 𝑥 𝑥
𝑏1 + 𝑏2 𝑚 = 0
The equation of the tangent or tangents at the origin is obtained by equating to zero
the terms of the lowest degree in the equation of the curve .
13.7 Condition for any Point (x, y) to be a Multiple Point of the Curve
f(x, y)=0
For a curve 𝑓(𝑥, 𝑦) = 0 ---- (1)
We can write
Therefore, to find the multiple points, we have to find the values of (𝑥, 𝑦) which simultaneously
satisfy the three equations:
𝑓𝑥 (𝑥, 𝑦) = 0
𝑓𝑦 (𝑥, 𝑦) = 0
𝑓(𝑥, 𝑦) = 0
𝑑𝑦
Differentiate 𝑓𝑥 + 𝑓𝑦 = 0 w.r.t. 𝑥, we get
𝑑𝑥
𝑑𝑦 𝑑2 𝑦 𝑑𝑦 2
𝑓𝑥𝑥 + 2𝑓𝑥𝑦 + 𝑓𝑦 2 + 𝑓𝑦𝑦 ( ) = 0
𝑑𝑥 𝑑𝑥 𝑑𝑥
𝑑𝑦
At the multiple points where 𝑓𝑦 = 0, 𝑓𝑥 = 0; the value of are the roots of the quadratic equation,
𝑑𝑥
𝑑𝑦 𝑑𝑦 2
𝑓𝑥𝑥 + 2𝑓𝑥𝑦 + 𝑓𝑦𝑦 ( ) = 0
𝑑𝑥 𝑑𝑥
In case 𝑓𝑥𝑥 , 𝑓𝑥𝑦 , 𝑓𝑦𝑦 are not all zero and 𝑓𝑥 = 0 = 𝑓𝑦 , the point (𝑥, 𝑦) will be a double point and will
be a
node if 𝒇𝟐𝒙𝒚 − 𝒇𝒙𝒙 𝒇𝒚𝒚 > 0
If 𝑓𝑥𝑥 = 𝑓𝑥𝑦 = 𝑓𝑦𝑦 = 0, the point (𝑥, 𝑦) will be a multiple point of the order higher than two,
those are not in the scope of this course.
∴ 𝑓𝑥 and𝑓𝑦 vanish at (0,0), (0, −𝑎), (𝑎, 0), (𝑎, −𝑎), (−𝑎, 0), (−𝑎, −𝑎).
Out of these, only (𝑎, 0), (−𝑎, 0)& (0, −𝑎) lie on the given curve.
Now 𝑓𝑥𝑥 = 12𝑥 2 − 4𝑎2
𝑓𝑦𝑦 = −12𝑎𝑦 − 6𝑎2
𝑓𝑥𝑦 = 0
We know,
𝑑𝑦 𝑑𝑦 2
𝑓𝑥𝑥 + 2𝑓𝑥𝑦 + 𝑓𝑦𝑦 ( ) = 0
𝑑𝑥 𝑑𝑥
At (𝑎, 0)
𝑑𝑦 2
−6𝑎2 ( ) + 4(2𝑎2 ) = 0
𝑑𝑥
√2
and at (0, −𝑎): 𝑦 + 𝑎 = ± 𝑥
√3
Alternatively,
We can find tangents at (𝑎, 0), by shifting the origin to (𝑎, 0) by following transformations,
𝑥 = 𝑋 + 𝑎, 𝑦 = 𝑌
⇒ 𝑋 + 4𝑋 𝑎 − 2𝑎𝑌 3 + 4𝑎2 𝑋 2 − 3𝑎2 𝑌 2 = 0
4 3
Locate the double points of the curve 𝑦(𝑦 − 6) = 𝑥 2 (𝑥 − 2)3 − 9 and mention their nature.
Here 𝑓(𝑥, 𝑦) = 𝑥 2 (𝑥 − 2)3 − 9 − 𝑦(𝑦 − 6) = 0
𝑓𝑥 = 𝑥(𝑥 − 2)2 (5𝑥 − 4)
𝑓𝑦 = 6 − 2𝑦
At (0, 3)
2 −𝑓 𝑓 < 0
𝑓𝑥𝑦 𝑥𝑥 𝑦𝑦
Summary
This chapter had variety of topics, which can be summarized as follows:
• Symmetry about the x-axis: In the function 𝑓(𝑥, 𝑦) = 0, replace 𝑦 with – 𝑦. If (𝑥, −𝑦) =
𝑓(𝑥, 𝑦) , then the graph will be symmetric about the x-axis.
• Symmetry about the y-axis: In the function 𝑓(𝑥, 𝑦) = 0, replace 𝑥 with – 𝑥. If (−𝑥, 𝑦) =
𝑓(𝑥, 𝑦) , then the graph will be symmetric about the y-axis.
• Symmetry about the origin: In the function 𝑓(𝑥, 𝑦) = 0, replace 𝑥, 𝑦 with – 𝑥, −𝑦. If
(−𝑥, −𝑦) = 𝑓(𝑥, 𝑦) , then the graph will be symmetric about the origin.
• Symmetry about the line, 𝑦 = 𝑥:In the function 𝑓(𝑥, 𝑦) = 0, replace 𝑥 with 𝑦 and 𝑦 with 𝑥.
If (𝑥, 𝑦) = 𝑓(𝑦, 𝑥) , then the graph will be symmetric about the line 𝑦 = 𝑥.
• Symmetry about the line, 𝑦 = −𝑥:In the function 𝑓(𝑥, 𝑦) = 0, replace 𝑥 with −𝑦 and 𝑦 with
−𝑥. If (𝑥, 𝑦) = 𝑓(−𝑦, −𝑥) , then the graph will be symmetric about the line 𝑦 = −𝑥.
• Symmetry in the opposite quadrants: In the function 𝑓(𝑥, 𝑦) = 0, replace 𝑥, 𝑦 with – 𝑥, −𝑦.
If (−𝑥, −𝑦) = 𝑓(𝑥, 𝑦) , then the graph will be symmetric in the opposite quadrants.
• Consider a function f(x) that is twice continuously differentiable on an interval I. The
function f(x) is concave upwards if f''(x) > 0 for all x in I and concave downwards if f''(x) <
0 for all x in I
• A point where a curve changes from concave upward to concave downward (or vice
versa), is called the inflexion point.
Keywords
Symmetry, lines of symmetry, concave up, concave down, convex, concave, point of inflection,
tangent at origin, multiple point, double point, node, cusp, isolated point
Self Assessment
1. How many lines of symmetry are there for a pentagon?
A. 2
B. 3
C. 4
D. 5
3. The curve 2𝑥 2 + 2𝑦 2 = 11 is
A. symmetric about the x-axis
B. symmetric about the y-axis
C. symmetric about the line y=x
D. all of the above
4. The notion of curvature of a graph upward or downward is known as
A. symmetry
B. asymptotes
C. concavity
D. multiple points
7. The point where a curve changes from concave upward to concave downward is called a
A. saddle point
11. For the curve 𝑥 3 + 𝑦 3 − 3𝑥𝑦 = 0, there exist ____ tangent(s) at the origin.
A. one
B. two
C. three
D. four
12. For the curve 𝑥 2 (𝑥 2 + 𝑦 2 ) = 5(𝑥 − 𝑦), the equation of the tangent at origin is
A. 𝑥 = 5𝑦
B. 𝑥 = −5𝑦
C. 𝑥 = −𝑦
D. 𝑥 = 𝑦
13. If the two tangents at a given point are not distinct, but coincide, we get
A. a node
B. a cusp
C. a conjugate point
D. none of these
14. If the curve lies entirely on one side of the common tangent (in the region of tangency),
the point is known as a
A. cusp of first kind
B. cusp of second kind
16. If at a point on a curve there exist two and only two distinct tangents, then that point is
called a
A. cusp of first kind
B. cusp of second kind
C. node
D. point of osculation
A. node
B. cusp
C. isolated point
D. none of these
A. node
B. cusp
C. isolated point
D. none of these
A. node
B. cusp
C. isolated point
D. none of these
6. A 7. D 8. A 9. C 10. A
Further Reading
W. Thomas Finny (1998). Calculus and Analytic Geometry, 6th Edition, Publishers, Narsa,
India.
R. K. Jain, and Iyengar, SRK. (2010). Advanced Engineering Mathematics, 3 rd Edition
Publishers, Narsa, India.
Widder, D.V. (2002). Advance Calculus 2nd Edition, Publishers, PHI, India.
Piskunov, N. (1996). Differential and Integral Calculus Vol I, & II, Publishers, CBS, India.
https://www.cuemath.com/geometry/symmetry/
https://math.libretexts.org/Bookshelves/Calculus/Book%3A_Calculus_(Apex)/03%3A_
The_Graphical_Behavior_of_Functions/3.04%3A_Concavity_and_the_Second_Derivative
https://schoolbag.info/mathematics/calculus_2/39.html
https://easy-to-understand-maths.blogspot.com/2019/03/multiple-point.html
Objectives
Students will be able to
Introduction
Can you recognize which of the following options depicts the curve x2y2(x+ y) = 1?
In order to answer the above question, we need to analyze the given Cartesian equation
thoroughly. An image is worth a thousand words. A curve which is the visual synonym of a
functionalrelation gives us the whole idea of information about the relation. Of course, we can also
obtain this information by analysing the equation which defines the functional relation. But
studying the associated curve is often easier and quicker. In addition to this, a curve which
represents a relation between two quantities also helps us to easily find the value of one quantity
Recall that, that the set of points {(x, y) : f(x, y) = 0) is known as the graph of the functional relation
f(x, y) = 0. Graphing a function or a functional relation means showing the points of the
corresponding set in a plane, thus, essentially curve tracing means plotting the points which satisfy
a given relation. However, there are some difficulties involved in this. Let's see what these are and
how to overcome them.
It is often not possible to plot all the points on a curve. The standard technique is to plot some
suitable points and to get a general idea of the shape of the curve by considering tangents,
asymptotes, singular points, extreme points, inflection points, concavity, monotonicity, periodicity
etc. Then we draw a free hand curve as nearly satisfying the various properties as is possible.
The curves or graphs that we draw have a limitation. If the range of values of either (or both)
variable is not finite, then it is not possible to draw the complete graph. In such cases the graph is
not only approximate, but is also incomplete. For example, consider the simplest curve, a straight
line. Suppose we want to draw the graph of 𝑓: 𝑅 → 𝑅such that𝑓(𝑥) = 𝑐. We know that this is in line
parallel to the x-axis. But it is not possible to draw a complete graph as the line extends infinitely on
both sides.
Suppose the equation of a curve is f(x, y) = 0.We shall now list some steps which, when taken, will
simplify our job of tracing this curve.
1. Domain
The first step is to determine the extentof the curve. In other words we try to find a region or
regions of the plane which cannot have any point of the curve. For example, no point on the curve
𝑥 = 𝑦 2 , lies in the second or the third quadrant, as the x-coordinate of any point on the curve has to
be non-negative. This means that our curve lies entirely in the first and the fourth quadrants.
Note thatit is easier to determine the extent of a curve if its equation can be written explicitly as y =
f(x) or x =f(y).
2. Intercepts
The next step is to determine the points where the curve intersects the axes. If we put y = 0 in f(x, y)
= 0, and solve the resulting equation for x, we get the points of intersection with the x-axis.
Similarly, putting x = 0 and solving the resulting equation for y, we can find the points of
intersection with the y-axis.
3. Symmetry
We find out if the curve is symmetrical about any line, or about the origin. We have already
discussed symmetry of curves in the previous unit. This step reduces our workload. If the curve is
symmetric about the x-axis, we can focus upon the region above x-axis only and then can replicate
that for the complete curve.
4. Asymptotes
The next step is to find the asymptotes, if there are any. They indicate the trend of the branches of
the curve extending to infinity. Asymptotes, if they exist, provide a frame for the curve.
Trace 𝑦 = 𝑥 3 − 12𝑥 − 16
Let us trace the curve step by step. For your ease the steps are mentioned below:
1. Domain
The function can take all real values of 𝑥 as its domain.
2. Intercepts
When 𝑥 = 0, 𝑦 = −16
When 𝑦 = 0, 𝑥 = −2, 4
Therefore the given curve meets the axes at (0, −16), (−2,0), (4,0).
3. Symmetry
No particular line of symmetry exists.
4. Asymptotes
No asymptote exists
5. Intervals of increase and decrease
𝑦 ′ = 3𝑥 2 − 12
𝑦 ′ = 0 ⇒ 𝑥 = ±2
∴ 𝑦 is increasing in (−∞, −2)
𝑦 is decreasing in (−2, 2)
𝑦 is increasing in (2, ∞)
6. Local maximum and minimum
𝑦 ′′ = 6𝑥
At 𝑥 = −2, 𝑦 ′′ < 0 ⇒ (−2, 0)is a point of maximum.
One advantage of using polar equations is that certain relations that are not functions in Cartesian
form can be expressed as functions in polar form.
Another advantage is that certain relations are much simpler to express in polar form rather than
Cartesian form.
• The curve is symmetric about the polar axis if for every point (r, θ) on the graph, the point
(r,−θ) is also on the graph. Similarly, the equation r=f(θ) is unchanged by replacing θ with
−θ
• The curve is symmetric about the pole if for every point (r, θ) on the graph, the point
(r,π+θ) is also on the graph. Similarly, the
equation r=f(θ) is unchanged when
replacing r with −r, or θ with π+θ.
• The curve is symmetric about the vertical
line θ=π/2 if for every point (r, θ) on the
graph, the point (r,π−θ) is also on the
graph. Similarly, the equation r=f(θ) is
unchanged when θ is replaced by π−θ.
2. Extent
∴ 𝑝 = 𝑟 cos(𝜃 − 𝛼)is the required equation of the line which is the prospective asymptote.
5. Region
Find the region in which the curve does not exist, or find the greatest and least numerical value of r
etc.
6. Specific points
Trace the variation of r as θ varies.
1. If we replace 𝜃to– 𝜃, the equation remains unchanged. So the given curve is symmetric
about the initial line.
2. The extent can be seen from the fact that maximum value of cos 𝜃is 1 and minimum value
is -1. Thus 𝑟 can take values from 0 to 2𝑎.
3. For 𝑟 = 0, we can see that𝜃 = 𝜋. This means that the curve passes through the pole.
4. Since it’s a polar curve we can find the value of 𝑟 at various 𝜃 values and then plot the
curve on a polar plane.
θ 0 𝜋 𝜋 𝜋 𝜋 2𝜋 𝜋
6 4 3 2 3
2𝑎 (√3 + 2) (√2 + 1) 3 𝑎 𝑎 0
𝑟 𝑎 𝑎 𝑎 2
2 √2 2
From all the above points, the following curve can be traced:
𝜃 0 𝜋 𝜋 3𝜋 2𝜋
2 2
𝑥 𝑎 0 −𝑎 0 𝑎
𝑦 0 𝑏 0 −𝑏 0
⇒ 𝑥=0
𝑑𝑦
When 𝜃 = 𝜋, =0
𝑑𝑥
⇒ 𝑥=0
Thus, the tangent at points (𝑎, 0)and (−𝑎, 0) is the x-axis and at the points (0, 𝑏)and (0, −𝑏) is the y-
axis.
And from this information we can draw the following:
𝜃 0 𝜋 −𝜋 3𝜋 −3𝜋
𝑥 0 𝑎𝜋 − 𝑎𝜋 3𝜋𝑎 −3𝜋𝑎
𝑦 2𝑎 0 0 0 0
𝑑𝑦
𝑑𝑦 𝑑𝜃 𝑑𝑥
= 𝑑𝑥
, ≠0
𝑑𝑥 𝑑𝜃
𝑑𝜃
𝑑𝑥
Here = 𝑎(1 + 𝑐𝑜𝑠𝜃)
𝑑𝜃
𝑑𝑦
= −𝑎 𝑠𝑖𝑛𝜃
𝑑𝜃
𝑑𝑦 𝜃
= − tan provided1 + 𝑐𝑜𝑠𝜃 ≠ 0 or 𝜃 ≠ ±𝜋
𝑑𝑥 2
When 𝜃 = 𝜋
The equation of the tangent is 𝑥 = 𝑎𝜋.
When 𝜃 = 0
The equation of the tangent is 𝑦 = 2𝑎.
Similarly the tangents at the other points can be checked and with the above information we can
trace the following:
Summary
• Steps for curve sketching of a Cartesian curve:
➢ Domain
➢ Intercepts
➢ Symmetry
➢ Asymptotes
➢ Intervals of Increase and Decrease
➢ Local Maximum and Minimum
➢ Concavity/Convexity and Points of Inflection
➢ Graph of the Function
➢ Steps for curve sketching of a polar curve:
➢ Symmetry
➢ Pole
➢ Asymptote
➢ Region
➢ Specific points
Keywords
Curve tracing, Cartesian curve, polar curve, parametric curve
Self Assessment
1. For the curve 𝑥 2 𝑦 2 (𝑥 + 𝑦) = 10 , which of the following is true?
A. The curve has an intercept on x-axis
B. The curve has an intercept on y-axis
C. The curve has an intercept on x-axis and y-axis
D. The curve has no intercept on x-axis and y-axis
6. The curve is symmetric about the polar axis if for every point (r, θ) on the graph, the point
(r, −θ) is also on the graph.
A. True
B. False
7. The curve is symmetric about the polar axis if for some point (r, θ) on the graph, the point
(r, −θ) is also on the graph.
A. True
B. False
8. The curve passes through the pole, if for r = 0, there corresponds a real value of θ.
A. True
B. False
6. A 7. B 8. A 9. C 10. A
Review Questions
Trace the following curves
1. 𝑦 2 = 8𝑥
2. 𝑥 2 + 𝑦2 = 9
3. 𝑥 2 𝑦 2 (𝑥 + 𝑦) = 10
4. 𝑥 3 + 𝑦 3 = 3𝑎𝑥𝑦
5. 𝑦 2 𝑥 2 = 𝑥 2 − 𝑎2
6. 𝑟 = 𝑎(1 + 𝑐𝑜𝑠 𝜃)
7. 𝑟 = 𝑎(1 − 𝑐𝑜𝑠 𝜃)
8. 𝑥 = 5 𝑐𝑜𝑠 3 𝜃, 𝑦 = 7 𝑠𝑖𝑛3 𝜃
9. 𝑟 = 𝑎 cos 2𝜃, 𝑎 > 0
10. 𝑟 = 𝑎 + 𝑏𝑐𝑜𝑠 𝜃
11. 𝑥 = 0.5 sec 𝑡, 𝑦 = 1 + cot 𝑡
12. 𝑥 = cos 𝑡, 𝑦 = cot 𝑡
13. 𝑟 log 𝜃 = 𝑎
14. 𝑟 = 𝑎(𝜃 − sin 𝜃)
15. 𝑟 = 𝑎 + 𝑎 sin 𝜃, 𝑎 > 0
https://maths4iitjee.page.tl/Curve-Tracing.htm
https://www.desmos.com/calculator/uu1erqkbey
https://www.kristakingmath.com/blog/sketching-polar-curves
https://brilliant.org/wiki/polar-curves/
https://math.libretexts.org/Bookshelves/Calculus/Map%3A_Calculus__Early_Transcen
dentals_(Stewart)/10%3A_Parametric_Equations_And_Polar_Coordinates/10.01%3A_Cu
rves_Defined_by_Parametric_Equations
https://tutorial.math.lamar.edu/classes/calcii/parametriceqn.aspx