Use the symmetries of the unit circle and of the sine, cosine and tangent graphs to relate values at θ, −θ, π − θ, π + θ and π/2 − θ, simplify expressions and find every solution of an equation.
IB Mathematics: Analysis and Approaches
Part of 3 Geometry and trigonometry
HL only
Key terms introduced here
Each is in the Maths AA glossary, with every other term in the subject.
A graph has point symmetry about a point M if a rotation of 180∘ about M maps the graph onto itself; M is the centre of symmetry.
Notes on 3.11 Symmetry of trigonometric graphs
20 min readLast reviewed
The graphs of sine, cosine and tangent are full of symmetry. The cosine curve is a mirror image of itself in the y-axis, the sine curve is unchanged by a half-turn about the origin, and each curve lands on itself after a translation by one period. Every one of these geometric facts is also an algebraic identity, such as cos(−θ)=cosθ or sin(π−θ)=sinθ, true for every angle θ.
These identities turn hard-looking expressions into simple ones, connect the sine and cosine functions to each other, and explain why the solutions of a trigonometric equation come in symmetric families. They are also the reason a single calculator value is enough to find every solution of an equation.
Symmetry in the unit circle
On the unit circle, the point at angle θ is P(cosθ,sinθ). Reflecting or rotating P in the axes and in the line y=x gives four more points whose angles are simple expressions in θ. Comparing their coordinates with those of P gives the symmetry relationships between the circular functions.
The four points at θ, π − θ, π + θ and −θ form a rectangle centred at O, so their coordinates differ only in sign. Reflecting in y = x swaps the two coordinates.
Transformation of P
New angle
New point
Relationship
Reflection in the x-axis
−θ
(cosθ,−sinθ)
cos(−θ)=cosθ, sin(−θ)=−sinθ
Reflection in the y-axis
π−θ
(−cosθ,sinθ)
sin(π−θ)=sinθ, cos(π−θ)=−cosθ
Rotation by π about O
π+θ
(−cosθ,−sinθ)
sin(π+θ)=−sinθ, cos(π+θ)=−cosθ
Reflection in y=x
2π−θ
(sinθ,cosθ)
cos(2π−θ)=sinθ, sin(2π−θ)=cosθ
Full turn
θ+2π
(cosθ,sinθ)
sin(θ+2π)=sinθ, cos(θ+2π)=cosθ
The tangent relationships follow by dividing the sine by the cosine in each row:
The figure is drawn with θ in the first quadrant, but the relationships hold for every angle. A reflection or rotation of the circle moves every point in the same way, whichever quadrant the point starts in, so the coordinates change in the same way too.
Negative angles: odd and even
Reflection in the x-axis changes the sign of the angle. The x-coordinate stays the same and the y-coordinate changes sign, so
cos(−θ)=cosθsin(−θ)=−sinθtan(−θ)=−tanθ
In the language of 2.14, cosine is an even function and sine and tangent are odd functions.
Line symmetry of the cosine graph
Because cos(−x)=cosx, the points (x,cosx) and (−x,cosx) are both on the graph of y=cosx. They are mirror images in the y-axis, so the whole graph is symmetrical about the y-axis.
y = cos x
The cosine graph is its own reflection in the y-axis: the points at θ and −θ are level with each other.
Point symmetry of the sine graph
Because sin(−x)=−sinx, the points (x,sinx) and (−x,−sinx) are both on the graph of y=sinx. The second is the image of the first after a rotation of 180∘ about the origin.
The graph of every odd function has point symmetry about the origin, and the graph of every even function has line symmetry in the y-axis. So the graphs of y=sinx and y=tanx have point symmetry about O, and the graph of y=cosx has line symmetry in the y-axis.
y = sin x
A half-turn about the origin maps the sine graph onto itself: the points at θ and −θ are the same distance from O on opposite sides.
Supplementary angles: π − θ
Reflection in the y-axis turns the angle θ into π−θ (in degrees, 180∘−θ). The height of the point does not change, but its horizontal coordinate changes sign:
sin(π−θ)=sinθcos(π−θ)=−cosθtan(π−θ)=−tanθ
The first of these is behind the rule "the second solution of sinx=k is π−α" used in 3.8.
Lines of symmetry of the sine graph
Replacing θ by 2π+t in sin(π−θ)=sinθ gives
sin(2π−t)=sin(2π+t)
The values of sinx at equal distances t either side of x=2π are the same, so the sine graph is symmetrical about the vertical line x=2π, which passes through its maximum. Because the graph repeats every 2π and is also symmetrical about the line through its minimum, it has a line of symmetry through every turning point: x=2π+kπ for every integer k.
y = sin x
The sine graph is symmetrical about the vertical line through each maximum and minimum, and has point symmetry about each zero, such as (π, 0).
The same reasoning applied to the other graphs gives a full list of their symmetries.
Graph
Lines of symmetry
Centres of symmetry
y=sinx
x=2π+kπ (through every maximum and minimum)
(kπ,0) (every zero)
y=cosx
x=kπ (through every maximum and minimum)
(2π+kπ,0) (every zero)
y=tanx
none
(2kπ,0) (every zero and every point where an asymptote meets the x-axis)
The centres of symmetry of the sine graph come from sin(π+t)=−sint and sin(π−t)=sint: together they give sin(π+t)=−sin(π−t), so the values at equal distances either side of x=π are equal in size and opposite in sign.
Half-turns and periods: π + θ
Rotating P through π about the origin turns θ into π+θ and changes the sign of both coordinates:
The last identity says that tan has period π. The first two say that translating the graph of y=sinx or y=cosx by π to the left gives the same result as reflecting it in the x-axis.
Combining the relationships gives others. For example, sin(θ−π) can be simplified by writing it as sin(−(π−θ)):
sin(θ−π)=−sin(π−θ)=−sinθ
using first that sine is odd and then the supplementary angle relationship. Alternatively, θ−π=(θ+π)−2π, so sin(θ−π)=sin(θ+π)=−sinθ.
Complementary angles: π/2 − θ
In a right-angled triangle, the two acute angles are complementary. The side opposite one of them is adjacent to the other, so the sine of each angle is the cosine of the other. The unit circle extends this to every angle: reflecting P in the line y=x swaps its coordinates and turns the angle θ into 2π−θ, so
sin(2π−θ)=cosθcos(2π−θ)=sinθtan(2π−θ)=tanθ1
The name cosine records this: the cosine of an angle is the sine of its complement. (The reciprocal tanθ1 is cotθ, defined in 3.9.)
Translating between sine and cosine graphs
Reading sin(x+2π)=cosx as a statement about graphs: translating the sine curve 2π to the left gives the cosine curve. In the same way cos(x−2π)=cos(2π−x)=sinx (cosine is even), so translating the cosine curve 2π to the right gives the sine curve. Any sinusoidal function can therefore be written using either sine or cosine.
y = sin x
y = cos x = sin(x + π/2)
Each feature of the sine curve, such as the maximum at (π/2, 1), appears on the cosine curve π/2 further left, at (0, 1).
Relationship
Graph statement
cosx=sin(x+2π)
y=cosx is y=sinx translated 2π to the left
sinx=cos(x−2π)
y=sinx is y=cosx translated 2π to the right
−sinx=cos(x+2π)
y=−sinx is y=cosx translated 2π to the left
−cosx=sin(x−2π)
y=−cosx is y=sinx translated 2π to the right
These translations are not the only ones that work. Because the graphs are periodic, adding any multiple of 2π to the translation gives the same result; for example, y=cosx is also y=sinx translated 23π to the right.
Using symmetry to simplify expressions
The relationships reduce the circular function of any angle of the form ±θ+2kπ to ±sinθ, ±cosθ or ±tanθ (or its reciprocal). Two checks decide the result:
Which function. Adding or subtracting π (or 2π) keeps the same function; adding or subtracting 2π (or 23π) swaps sine and cosine.
Which sign. Imagine θ as a small positive acute angle, find the quadrant of the new angle, and use the sign of the original function in that quadrant.
For example, for cos(23π+θ): the 23π swaps cosine to sine; with θ small, 23π+θ is in the fourth quadrant, where cosine is positive. So cos(23π+θ)=sinθ.
Expressions with several terms are simplified term by term, then collected.
Pairs of terms that are complementary or supplementary often cancel or combine, which is useful for sums with many terms.
Using symmetry to find all solutions
Every solution of a trigonometric equation is related to every other by a symmetry of the graph. Once one solution is known, the lines of symmetry give a second, and the period gives the rest.
Symmetry of a transformed graph
For a transformed function such as f(x)=asin(bx)+d, the lines of symmetry move with the graph. They pass through the maxima and minima, which for sin(bx) are at bx=2π+kπ, that is x=2bπ+bkπ. If x1 is a solution of f(x)=k, its reflection in the nearest line of symmetry x=m is 2m−x1, which is also a solution.
Equations of the form sin A = sin B and cos A = cos B
The symmetry relationships also say exactly when two angles have the same sine or the same cosine. The angles B and π−B have the same sine, and so does any angle a whole number of turns away from either. Similarly, B and −B have the same cosine, and the tangent repeats every π:
sinA=sinB⟺A=B+2kπ or A=π−B+2kπ
cosA=cosB⟺A=B+2kπ or A=−B+2kπ
tanA=tanB⟺A=B+kπ
where k∈Z. These give every solution of an equation in which the same function is applied to two different expressions.
When the two sides use different functions, a complementary angle relationship makes them the same function first.
Exam-style questions on symmetry of trigonometric graphs
The second question combines symmetry with a known exact value.
Self-check
To do:
I can derive the relationships for −θ, π−θ, π+θ and 2π−θ from reflections and rotations of the unit circle.
To do:
I can explain that cosine is even and sine and tangent are odd, and what this means for their graphs.
To do:
I can state the lines of symmetry and centres of symmetry of the sine, cosine and tangent graphs.
To do:
I can write a sine graph as a translation of a cosine graph, and the reverse, including for sin(bx) and cos(bx).
To do:
I can simplify expressions such as cos(23π+θ) by deciding the function and the sign.
To do:
I can use complementary and supplementary angles to evaluate sums and exact values.
To do:
I can find a second solution of an equation by reflecting a known solution in a line of symmetry.
To do:
I can solve equations of the form sinA=sinB and cosA=cosB by considering both cases.
Questions on 3.11
15 exam-style questions on this subtopic, written in the style of the IB papers. The first has its markscheme open. Counted on
Question 1 · AA-001877 marks
It is given that sin9π=p, where 0<p<1.
(a)(i)
Write down, in terms of p, the value of sin98π.
[1]1 mark
Markscheme (a)(i)
sin98π=sin(π−9π)=pA1
(a)(ii)
Write down, in terms of p, the value of sin910π.
[1]1 mark
Markscheme (a)(ii)
sin910π=sin(π+9π)=−pA1
(b)
Find, in terms of p, the value of cos1811π.
[2]2 marks
Markscheme (b)
cos1811π=cos(2π+9π)(M1)
=−sin9π=−pA1
Note: Accept use of the compound angle identity for the (M1).
(c)
Find, in terms of p, the value of tan917π.
[3]3 marks
Markscheme (c)
cos9π=1−p2 (positive since 9π is acute) (A1)
tan917π=tan(2π−9π)=−tan9π(M1)
=−1−p2pA1
Note: Award (A1)(M1)A0 for 1−p2p.
Question 2 · AA-001887 marks
Let α be the solution of the equation cosx=0.35 for which 0<α<2π.
(a)
Find the value of α.
[1]1 mark
(b)
Write down, in terms of α, the four solutions of cosx=0.35 for −2π≤x≤2π.
A large observation wheel rotates at a constant speed. The height, h metres, of a capsule above the ground t minutes after it passes the lowest point of the wheel is modelled by
h(t)=20−18cos(15πt),t≥0.
(a)
Write down the time taken for the wheel to complete one rotation.
[1]1 mark
(b)
The model can also be written in the form h(t)=18sin(15π(t−q))+20, where q>0. Find the smallest possible value of q.
[3]3 marks
(c)
Find the first time at which the capsule is 30 metres above the ground.
[2]2 marks
(d)
By using the symmetry of the graph of h, find the length of time, during each rotation, for which the capsule is more than 30 metres above the ground.