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The document discusses line integrals, focusing on their evaluation over curves in two-dimensional and three-dimensional spaces, involving scalar and vector fields. It provides definitions, examples, and techniques for expressing integrals in terms of a single variable, along with specific examples illustrating the evaluation of line integrals. Additionally, it touches on double integrals and the importance of the order of integration, emphasizing that the results remain consistent regardless of the order chosen.
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Save Mts 201. Line Integral (1) For Later 1. Line integrals
HELM 28 was concerned with evaluating an integral over all points within a rectangle or other shape
(or over a cuboid or other volume). In a related manner, an integral can take place over a line or
curve running through a two-dimensional (or three-dimensional) region. Line integrals may involve
scalar or vector fields. Those involving scalar fields are dealt with first
Line integrals in two dimensions
A line integral in two dimensions may be written as,
[Pevdw
‘There are three main features determining this integral:
F(z.y): This is the scalar function to be integrated eg. F (x,y) =x? + 4y”
2 ofr =siny
 
 
c This is the curve along which integration takes place. e.g.
orr=t~1; y=? (where x and y are expressed in terms of a parameter t)
dw: This gives the variable of the integration. Three main cases are dr, dy and ds
Here ‘s’ is arc length and so indicates position along the curve C.
7
ds may be written as ds = /(dr)? + (dy)? or ds = \/1+ (#) de
A fourth case is when F(x.) dw has the form: Fydr-+Fxdy. This is a combination
of the cases dir and dy.
The integral f F(.c.y) ds represents the area beneath the surface z = F(z,y) but above the curve
c
The integrals / F(r,y) dr and f F(z,y) dy represent the projections of this area onto the x=
and yz planes respectively. ,
A particular case of the integral f F(z, y) da is the integral f 1 ds. This is a means of calculating
   
 
the length along a curve ie. an arc length
Sele
 
 
Figure 1; Representation of a line integral and its projections onto the .x and y2 planes
HELM (2008)
Section 29.1: Line IntegralsThe technique for evaluating a line integral is to express all quantities in the integral in terms of a
single variable. If the integral is with respect to ‘zx’ or ‘y', then the curve 'C’ and
the function 'F' may be expressed in terms of the relevant variable. If the integral is with
respect to ds, normally all quantities are expressed in terms of x. If xr and y are given in terms of a
parameter ¢, then ¢ is used as the variable
 
Example 1
Find fea +4y)dx where Cis the curve y =x”, starting from x = 0,y=0
and ending at x= l,y
 
 
 
Solution
As this integral concerns only points along C and the integration is carried out with respect to =r,
y may be replaced by 2?. The limits on x will be 0 to 1. So the integral becomes
 
 
 
 
i x(l+4y)dr =
ie
i =
l
Example 2
Find Prasan dy where C is the curve y starting from
2=0,y=0 and ending at x= 1,y = 1. Thisis the same as Example 1 other
    
than dz being replaced by dy,
 
 
Solution
 
AAs this integral concerns only points along C’ and the integration is carried out with respect to y,
everything may be expressed in terms of y, i.e. x may be replaced by y'/?, The limits on y will
be 0 to 1, So the integral becomes
feo+m dy
lc
  
 
 
 
 
4 HELM (2008)
Workbook 29: Integral Vector Calculus» Example 3
Find | r(1+4y)ds where C is the curve y =
   
starting from r = 0,y =0
and ending at x = 1,y= 1. This is the same integral and curve as the previous
two examples but the integration is now carried out with respect to s, the arc
length parameter
 
 
Solution |
As this integral is with respect to .r, all parts of the integral can be expressed in terms of x, Along
2 |
fis (¥) da = \/14 (20)'de = V1 4dr |
ds
  
y
So, the integral is
1
1
feasanas= [ x (1+ 42?) VIET de = [ (14407)? de
F 0
fe=0) |
This can be evaluated using the transformation u=1+42? so du =8cdr ie. cdr = Fz
When x= 0, w=1 and when x=1, u=5
Hence,
‘
ie _
 
x? wr)’ 22 pps a) 2.745 i
5 20 ° |
 
 
Note that the results for Examples 1,2 and 3 are all different: Example 3 is the area between a curve
and a surface above; Examples 1 and 2 give projections of this area onto other planes.
Example 4
Find [ xy dx where, on C, x and y are given in terms of a parameter t by
ie
£3 — 1 for t varying from 0 to 1
 
r= 3ty
 
 
 
Solution
Everything can be expressed in terms of ¢, the parameter. Here x = 31? so di = 6t dt. The limits
ont are t= 0 and t= 1. The integral becomes
[wae =
  
 
 
 
 
HELM (2008) 5
Section 29.1: Line IntegralsWB key Point 1
A line integral is normally evaluated by expressing all variables in terms of one variable.
In general
[senase f sew ave [ fe) ae
   
For F(z,y) = 20 +9, find (i) f Fle) ae, ( [Fen dy,
(iii) [ F (x,y) ds where C is the line y = 2 from (0,0) to (1,2).
le
Express each integral as a simple integral with respect to a single variable and hence evaluate each
integral
 
Your solution
 
 
 
 
 
Answer
@ [ere dr = i (ii) for WP) dy
(iii) fe be?) V5 dl
a
 
 
<
 
 
6 HELM (2008):
Workbook 29: Integral Vector CalculusHEL VARS
Find () [Fee y) de, (i) [Few y) dy, ci fx (2,y) ds where F(r,y) = 1
and C is the curve y = 1? — 4 na from (1, 4) to (2,2 ~ #1n2)
 
 
 
Your solution
 
 
 
 
 
Answer
som
maaan ¢ wf dy=3—2in2, tii) y=}
dy
de
lds= Lee pear | festa = fice dyed
2 ae 274
 
 
 
Find () [| Flew) dz, (i) [Few dy, (iii [Fen ds
where F(z,y) = sin 2x and C is the curve y = sinz from (0,0) to Ga)
 
Your solution
 
 
 
 
 
 
Answer
xf =) 2
of sin2cdr=1, (i [ 2sin x cos? x de= 5
0 0
 
sf .
(iii) [ sin2eV1+ cos? x de = 3(2v2 ~ 1), using the substitution u = 1 + cos? x
5
HELM (2008)
Section 29.1: Line IntegralsNIG A
Calculus mt
 
Example I Compute each of the following double integrals over the indicated rectangles.
(a) [f6xv° dd, R=[2,4]x[1,2] (Solution
(b) ff2x-4y°d4. R=[-5.4]x[0.3] [Solution
(©) [fx°y* +c08(zx)+sin(zy)d4, R=[-2,-1]x[0,1] {Solution
fk
@) las“ R=[0.1}x[1,2] (Solution)
© [eer au, R=[-1,2]x[0.1] {Solution}
Solution
(a) f[6x* a4, R=[2,4]x[1,2]
f
It doesn’t matter which variable we integrate with respect to first, we will get the same answer
regardless of the order of integration. To prove that let's work this one with each order to make
sure that we do get the same answer.
Solution 1
In this case we will integrate with respect to y first. So, the iterated integral that we need to
compute is,
foo? t= foo? aa
When setting these up make sure the limits match up to the differentials. Since the dy is the inner
differential (i, we are integrating with respect to y first) the inner integral needs to have y limits,
To compute this we will do the inner integral first and we typically keep the outer integral around
as follows,
47 yp
fis ;
{fo a= fi (2x i a&
‘
=|, 16x-2x¢x
=[l4xde
= fyi
Remember that we treat the x as a constant when doing the first integral and we don’t do any
integration with it yet. Now, we have a normal single integral so let's finish the integral by
computing this.
Jf oo? a4=73" f 84
 
 
 
© 2007 Paul Dawkins 9 httpi/tutorial.math.lamar.edu/terms.aspx
oeCalculus 111
 
‘Solution 2 : ;
In this case we'll integrate with respect to x first and then y. Here is the work for this solution.
[Joo dae [fio day
J
=[oev eo
=f 36)? a
e
=12y'|
=84
Sure enough the same answer as the first solution,
So, remember that we can do the integration in any order.
(Return to Problems)
(b) ff2x-4y'aa, R=[-5.4]x([0,3]
For this integral we'll integrate with respect to y first.
cael
[fox-ay' aa f Jp2x-4y' dae
® Ss
= f.e0-y" Jae
‘
= [/,6x-81de
=(3x*-81x)|)
=-756
 
Remember that when integrating with respect to y all x’s are treated as constants and so as far as
the inner integral is concerned the 2x is a constant and we know that when we integrate constants
with respect to y we just tack on a y and so we get 2xy from the first term.
[Return to Problems]
(©) [[2y? +cos(ax)+sin(zy)da, R=[-2,-1]x(0,1]
 
 
In this case we'll integrate with respect to x first.
 
© 2007 Paul Dawkins 10 hhttp:/tutorial.math,lamar.edu/terms.aspxCaleulus It
 
i
fey +cos(x)+sin(y)da= fff x°y? +00s (mx) +sin(ny)dedy
‘1
Lay
=| [S°7+
[Gers
a
=| Zy+sin(xy) a
fb sin(my)dy
a
dy
la
 
in(ax)+xsin(xy)]
 
 
Don't forget your basic Calculus | substitutions!
(Return 0 Problems}
@ lm R=([0.1]x[1,2]
Inthis case because the limits for x are kind of nice (ie. they are zero and one which are often
tase for evaluation) let's integrate with respect to x first. We'll also rewrite the integrand to help
with the first integration.
(forssyy ate f[laxea) dey
-[ Gown]
ke
ay
 
 
 
[Return to Problems]
(© [fxe? 44, R=[-1,2]x(0.1]
  
Now, while we can technically integrate with respect to either variable first sometimes one way is
significantly easier than the other way. In this case it will be significantly easier to integrate with
respect to y first as we will see. |
 
 
© 2007 Paul Dawkins " hhttp:/tutorial. math.lamar.edu/terms.aspxi
: " ees
[fxr a4=f? fre” ava
| The y integration can be done with the quick substitution,
| u=xy du = xdy
which gives
2
[rer at= [orl ae
maa
‘
=f) et-ldr
 
So, not too bad of an integral there provided you get the substitution. Now let’s see what would
happen if we had integrated with respect to x first.
1
[fs = [fe a
In order to do this we would have to use integration by parts as follows,
dv=e” de
   
‘The integral is then,
We're not even going to continue here as these are very difficult integrals to do.
{Return to Problems]
 
‘As we saw in the previous set of examples we can do the integral in either direction. However,
sometimes one direction of integration is significantly easier than the other so make sure that you
think about which one you should do first before actually doing the integral.
The next topic of this section is a quick fact that can be used to make some iterated integrals
somewhat easier 1o compute on occasion
© 2007 Paul Dawkins 2 ‘http:/tutorial math. lamar.edu/terms.aspxnas
 
Fact
f(y)
 
 
= g(x)h(y) and we are integrating over the rectangle R= [a,b}x[e.d]
[Jr@.y)aa = [feG)H(vya=(fFxCo)as)( ya)
then,
— ih it
 
So, if we can break up the function into a function only of x times a function of y then we can do
the two integrals individually and multiply them together.
Let’s do a quick example using this integral
 
 
Example 2 Evaluate [{.xcos? (y)dd, R=
f
230
 
Solution
Since the integrand is a function of x times a function of y we can use the fact.
[J>eos (yaa -({4[ J 3 cos? (ya)
se 0
 
 
We have one more topic to discuss in ction. This topic really doesn’t have anything to do
with iterated integrals, but this is as good a place as any to put it and there are liable to be some
questions about it at this point as well so this is as good a place as any,
 
‘What we want to do is discuss single indefinite integrals of a function of two variables. In other
words we want to look at integrals like the following,
Jxse
-e'dy
 
 
2y)+4aydy
 
From Calculus | we know that these integrals are asking what function that we differentiated to
get the integrand, However, in this ease we need to pay attention to the differential (dy or cx) in
the integral, because that will change things a little
 
 
In the case of the first integral we are asking what function we differentiated with respect tov to
get the integrand while in the second integral we're asking what function differentiated with
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be ae fo
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N a(t +3) ze ——.
Uy ww BA+3~0
=) eee leatCalculus Itt
 
(0) [f4xv-y' dA, Dis the region bounded by y= Vx and y =x
In this case we need to determine the two inequalities for x and y that we need to do the integral.
The best way to do this is the graph the two curves. Here is a sketch.
y
1
og
06
 
  
 
oa)
02
02 04~=—O06SsC 1
‘So, from the sketch we can see that that two inequalities are,
Osx! x 
a&
 
4
   
I J 35
tox} =
52” J, 156
[Return to Problems]
(©) [J}6x" 40d, Dis the triangle with vertices (0,3), (1,1), and (5,3).
We got even less information about the region this
triangle,
 
ime. Let's start this off by sketching the
 
 
© 2007 Paul Dawkins ‘http:/tutorial.math.lamar.edw/terms.aspx2
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eet fat , ee
eb
cS fant, 46 fanehin, F (4, yt) + [Poy 2), RO4y, By Ror, yt
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