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Mod 2 Pure

The document covers key concepts in trigonometry, coordinate geometry, and vectors in three dimensions. It includes graphs and general solutions for trigonometric functions, equations and properties of circles, ellipses, and parabolas, as well as vector equations for lines and planes. Essential identities and equations for each topic are provided for reference.

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Megan Jawahir
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0% found this document useful (0 votes)
27 views3 pages

Mod 2 Pure

The document covers key concepts in trigonometry, coordinate geometry, and vectors in three dimensions. It includes graphs and general solutions for trigonometric functions, equations and properties of circles, ellipses, and parabolas, as well as vector equations for lines and planes. Essential identities and equations for each topic are provided for reference.

Uploaded by

Megan Jawahir
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
Available Formats
Download as PDF, TXT or read online on Scribd
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MODULE 2tCHAPTER 9

SUMMARY
Trigonometry

Graphs and general solutions Trigonometric identities

Graph of y = sin x sin2 θ + cos2 θ = 1


y
1 tan2 θ + 1 = sec2 θ
1 + cot2θ = cosec2θ
x
0 π π 3π 2π
2 2

–1
sin (A ± B) = sin A cos B ± cos A sin B
cos (A ± B) = cos A cos B ∓ sin A sin B
tan (A ± B) = tan A ± tan B
– tan A tan B
Graph of y = cos x 1+
y
1

x sin 2θ = 2 sin θ cos θ


0 π π 3π 2π cos 2θ = cos2θ – sin2θ
2 2
cos 2θ = 2 cos2θ – 1
–1 cos 2θ = 1 – 2 sin2θ
tan 2θ = 2 tan θ2
1 – tan θ
Graph of y = tan x
y

1
If t = tan θ , then:
x 2
π π
sin θ = 2 2t
– 0
2 2
t +1
–1
cos θ = 1 – t 2
2

1+t
tan θ = 2t 2
Graph of y = cosec x 1–t
y

1
x
2sin A cos B = sin (A + B) + sin (A – B)
0 π 2π 2cos A sin B = sin (A + B) – sin (A – B)
–1
2cos A cos B = cos (A + B) + cos (A – B)
–2sin A sin B = cos (A + B) – cos (A – B)

Graph of y = sec x sin A + sin B = 2sin A + B cos A – B


y
2 2
sin A – sin B = 2cos A + B sin A – B
2 2
cos A + cos B = 2cos A + B cos A – B
1
x
0 π π 3π 2 2
cos A – cos B = –2 sin A + B sin A – B
–1 2 2
2 2

a cos θ + b sin θ ≡ r cos θ


Graph of y = cot x where r > 0 and 0° < α < 90°
y

x Maximum (a cos θ + b sin θ ) = r,


–π 0 π
when cos (θ – α) = 1

Minimum (a cos θ + b sin θ ) = –r,


General solution of sin x: when cos(θ – α) = –1
x = nπ + (–1)nα, n ∈

General solution of cos x:


x = 2nπ ± α, n ∈

General solution of tan x:


x = nπ + α, n ∈

263
MODULE 2tCHAPTER 10

SUMMARY
Coordinate geometry

Circles Ellipses Parabolas

A circle is the locus of a point An ellispse is the locus of points, A parabola is a set of all points in a plane, which
which moves in a plane so that the sum of whose distance from two are at the same distance from a fixed point P as
it is equidistant from a fixed fixed points is constant. The two fixed they are from a fixed line l. P is called the focus
point. points are the foci of the ellipse. and l is called the directrix.

Equation of a circle centre (0, 0) Equation of an ellipse with centre (0, 0) Equation of a parabola with centre
and radius r : and foci at (c, 0) and (–c, 0) is: (0, 0) and opening upwards is:
x2 + y2 = r2 x2 + y2 = 1 x2 = 4ay
a2 b2
Equation of a circle centre (a, b) Equation of a parabola with centre
and radius r : Equation of an ellipse with foci (0, c) (0, 0) and opening to the right is:
(x – a)2 + (y – b)2 = r2 and (0, –c) is: y2 = 4ax
x2 + y2 = 1
a2 b2
General equation of a circle: Equation of a parabola with axis of symmetry
Ax2 + By2 + Cx + Dy + E = 0, A = B Equation of an ellipse with centre parallel to the y-axis is:
(h, k) and major axis parallel to the y = ax2 + bx + c a ≠ 0
x-axis is:
(x – h)2 (y – k)2 Equation of a parabola with axis of symmetry
+ =1
(a, b) a2 b2 parallel to the x-axis is:
r Foci are at (h + c, k) and (h – c, k). x = ay2 + by + c a ≠ 0

Equation of an ellipse with centre Equation of a parabola in vertex form:


Parametric equation of a circle (h, k) and major axis parallel to the y = a(x – h)2 + k
centre (a, b) and radius r : y-axis is: or y = a(y – k)2 + h
x = a + r cos θ y = b + r sinθ (x – h)2 (y – k)2
+ =1
or x = a + r sinθ y = b + r cosθ b2 a2 Equation of a parabola in conics form:
Foci are at (h, k + c) and (h, k – c).
4p(y – k) = (x – h)2
Gradient of the normal at or 4p(x – h) = (y – k)2
y –b
P= 0 General equation of an ellipse:
x0 – a
Ax2 + B2 + Cx + Dy + E = 0, A ≠ B where p is the distance from the vertex
to the focus (also the distance from the
Graph of an ellipse centre C, vertex to the directrix).
P foci F1 and F2 (2p is the distance from the focus to
(a, b) (x0 , y0)
r the directrix).
Minor axis

Axis of symmetry
Since the tangent is perpendicular Major
V2 Centre V1 P
to the radius, the gradient of the F1 F2 axis d
y –b d F
tangent of P is –( 0 ) a
x0 – a a
V
Dir
Given three points on a ect
rix
circle we can find its equation ,D
Parametric equations of an ellipse centre
by using the general form
(h, k) and radius r :
(x – a)2 + (y – b)2 = r2.
x = h + a cos t y = k + b sin t
We form three equations Parametric equations of a parabola are:
and solve them simultaneously x = at2 y = 2at t ∈ a>0
to find a, b and r. Gradient of the tangent at
P(a cos t, b sin t) is
Gradient of the tangent to a parabola
Or, if the circle passes –b cos t 1
through P, Q and R, the a sin t at P(at2, 2at) is t
centre of the circle is the and the gradient of the normal is
point of intersection of the a sin t
Gradient of the normal to a parabola at
perpendicular bisectors b cos t
P(at2, 2at)) is – t.
of PQ and QR. The radius
can be found using the
centre and any of the Equation of the tangent can be found
points P, Q and R. by using the gradient and point.

299
M O DUL E 2
SUMMARY
Vectors in three dimensions ( 3)

Vectors Lines Planes

u1 v1 Let a be a point on a line and m be Let nˆ be a unit vector perpendicular to a


Let u = u2 and v = v2 the direction vector. The equation of plane and d be the distance from the
u3 v3 origin to the plane. The equation of the
the line is
plane is:
r = a + λm, λ ∈ r ⋅ nˆ = d
u1 + v1
u2 + v2 Let p and q be two points on a line.
u+v=
u3 + v3 The equation of the line is
λ λ Let a be a point on a plane and n a vector
perpendicular to the plane. The equation
of the plane is:
u1 – v1 Vector equation of a line: r⋅n=a⋅n

u−v= u2 – v2 a x0
u3 – v3 r= b +λ y0
c z0 Vector equation of a plane:
A

u1 λu1 r. B ∙D
Cartesian equation of a line:
λu2 C
λ u2 = , λ∈ x–a y–b z–c
= =
u3 λu3 x0 y0 z0

Cartesian equation of a plane:


u = v iff u1 = v1, u2 = v2, u3 = v3 Parametric equations of a line:
Ax + By + Cz = D
x = a + λ x0
A
u · v = u1v1 + u2v2 + u3v3 y = b +λ y0 λ ∈
where B is a vector perpendicular to
z = c + λ z0 C
u = u12 + u22 + u32 the plane.

Skew lines are lines that are not


A unit vector is a vector with
parallel and do not intersect.
magnitude 1 unit.

The angle between two lines is the


A unit vector in the direction of u is angle between their direction vectors.
u .
|u|
Two lines are perpendicular iff the
u · v = |u||v| cos θ , where θ is the scalar product of their direction
angle between u and v. vectors is 0.

u and v are perpendicular iff u · v = 0.

u and v are parallel iff one is a scalar


multiple of the other.

1 0 0
i= 0 , j= 1 , k= 0
0 0 1

a
b = ai + bj + ck
c

334

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