A-level Mathematics

5.9 The forms r cos(theta +/- alpha) and r sin(theta +/- alpha) — Learn

Prerequisites: the addition formulae; exact values; solving a simple trigonometric equation; Pythagoras' theorem.

By the end of this section you can: write acos⁡θ+bsin⁡θa\cos\theta + b\sin\theta as a single cosine or sine; find its greatest and least values; use the form to solve an equation.

1. One wave from two

A sum of a cosine and a sine of the same angle is itself a single wave. For constants aa and bb,

acos⁡θ+bsin⁡θ≡Rcos⁡(θ−α),a\cos\theta + b\sin\theta \equiv R\cos(\theta - \alpha),

where

R=a2+b2,tan⁡α=ba.R = \sqrt{a^2 + b^2}, \qquad \tan\alpha = \frac{b}{a}.

The value of RR comes from expanding the right-hand side with the addition formula:

Rcos⁡(θ−α)=Rcos⁡θcos⁡α+Rsin⁡θsin⁡α.R\cos(\theta - \alpha) = R\cos\theta\cos\alpha + R\sin\theta\sin\alpha.

Matching this with acos⁡θ+bsin⁡θa\cos\theta + b\sin\theta gives

a=Rcos⁡α,b=Rsin⁡α.a = R\cos\alpha, \qquad b = R\sin\alpha.

Squaring and adding these two equations gives a2+b2=R2a^2 + b^2 = R^2, so R=a2+b2R = \sqrt{a^2 + b^2}. Dividing the second by the first gives tan⁡α=ba\tan\alpha = \dfrac{b}{a}.

The angle α\alpha must lie in the quadrant where cos⁡α\cos\alpha has the sign of aa and sin⁡α\sin\alpha has the sign of bb. The single value returned by arctan⁡\arctan is not always the right one, so check the signs of aa and bb.

You can also write the same sum as a shifted sine:

acos⁡θ+bsin⁡θ≡Rsin⁡(θ+β),a\cos\theta + b\sin\theta \equiv R\sin(\theta + \beta),

where R=a2+b2R = \sqrt{a^2 + b^2} and sin⁡β=aR\sin\beta = \dfrac{a}{R}, cos⁡β=bR\cos\beta = \dfrac{b}{R}.

2. The greatest and least values

Because a cosine lies between −1-1 and 11,

−R≤Rcos⁡(θ−α)≤R.-R \le R\cos(\theta - \alpha) \le R.

So the greatest value of acos⁡θ+bsin⁡θa\cos\theta + b\sin\theta is RR, and the least value is −R-R. This is useful in modelling: the single number RR gives the peak of the quantity without drawing a graph.

Example 1. Write 3cos⁡θ+4sin⁡θ3\cos\theta + 4\sin\theta in the form Rcos⁡(θ−α)R\cos(\theta - \alpha), where α\alpha is an acute angle.

R=32+42=25=5.R = \sqrt{3^2 + 4^2} = \sqrt{25} = 5. tan⁡α=43,α≈0.9273 radians.\tan\alpha = \frac{4}{3}, \qquad \alpha \approx 0.9273 \text{ radians}.

Both 33 and 44 are positive, so α\alpha is acute and the angle from the calculator is correct. Therefore

3cos⁡θ+4sin⁡θ=5cos⁡(θ−0.9273).3\cos\theta + 4\sin\theta = 5\cos(\theta - 0.9273).

The greatest value is 55 and the least is −5-5.

Example 2. Write −cos⁡θ+3sin⁡θ-\cos\theta + \sqrt{3}\sin\theta in the form Rcos⁡(θ−α)R\cos(\theta - \alpha).

R=(−1)2+(3)2=4=2.R = \sqrt{(-1)^2 + (\sqrt{3})^2} = \sqrt{4} = 2.

Here a=−1a = -1 and b=3b = \sqrt{3}. The angle α\alpha must have a negative cosine and a positive sine, so it lies in the second quadrant. The related acute angle is arctan⁡(3)=π3\arctan(\sqrt{3}) = \dfrac{\pi}{3}, so

α=π−π3=2π3.\alpha = \pi - \frac{\pi}{3} = \frac{2\pi}{3}.

Therefore

−cos⁡θ+3sin⁡θ=2cos⁡(θ−2π3).-\cos\theta + \sqrt{3}\sin\theta = 2\cos\left(\theta - \frac{2\pi}{3}\right).

3. Solving an equation with the single-wave form

The single-wave form turns acos⁡θ+bsin⁡θ=ca\cos\theta + b\sin\theta = c into one cosine equation, which is much easier to solve.

Example 3. Solve 3cos⁡θ+4sin⁡θ=23\cos\theta + 4\sin\theta = 2 for 0≤θ<2π0 \le \theta < 2\pi.

From Example 1, the left-hand side is 5cos⁡(θ−0.9273)5\cos(\theta - 0.9273). So

5cos⁡(θ−0.9273)=2,cos⁡(θ−0.9273)=0.4.5\cos(\theta - 0.9273) = 2, \qquad \cos(\theta - 0.9273) = 0.4.

The principal value is cos⁡−1(0.4)≈1.1593\cos^{-1}(0.4) \approx 1.1593 radians. Cosine is also positive at the negative of this angle, so

θ−0.9273≈1.1593orθ−0.9273≈−1.1593.\theta - 0.9273 \approx 1.1593 \quad \text{or} \quad \theta - 0.9273 \approx -1.1593. θ≈2.0866orθ≈−0.2320.\theta \approx 2.0866 \quad \text{or} \quad \theta \approx -0.2320.

Only the first lies in 0≤θ<2π0 \le \theta < 2\pi. The second is negative, so add 2π2\pi:

θ≈−0.2320+6.2832=6.0512.\theta \approx -0.2320 + 6.2832 = 6.0512.

The solutions are θ≈2.087\theta \approx 2.087 and θ≈6.051\theta \approx 6.051.

4. Try it: the single-wave explorer

Predict first. You will change aa and bb in acos⁡θ+bsin⁡θa\cos\theta + b\sin\theta. Before you touch the controls, predict what the greatest value becomes when a=3a = 3 and b=4b = 4, and whether changing the sign of bb moves the peak left or right. Write both predictions down.

Test. Move the sliders and watch the sum wave. Compare the peak height with the value of RR in the readout. Set a=0a = 0 and check that the result is a pure sine wave.

Explain. Write two sentences. The first explains why the peak height depends on both aa and bb through R=a2+b2R = \sqrt{a^2 + b^2}. The second explains why the peak slides along the θ\theta-axis when bb changes.

Watch out. Two mistakes are common with the single-wave form.

Using the wrong quadrant for α\alpha. The calculator gives one angle for tan⁡α=ba\tan\alpha = \dfrac{b}{a}. If aa is negative, the true α\alpha is in the second or third quadrant, not the one a calculator returns by default. Check the signs of aa and bb and adjust α\alpha by π\pi when needed.

Mixing up the forms. In Rcos⁡(θ−α)R\cos(\theta - \alpha), the matching gives a=Rcos⁡αa = R\cos\alpha and b=Rsin⁡αb = R\sin\alpha. In Rsin⁡(θ+β)R\sin(\theta + \beta) the roles swap. Decide which form the question asks for before you match coefficients.

Re-check: expand your answer with the addition formula and confirm that the coefficients of cos⁡θ\cos\theta and sin⁡θ\sin\theta match the original aa and bb.

Progress check

Return to the chapter problem. The tide height is h=12cos⁡θ+5sin⁡θh = 12\cos\theta + 5\sin\theta metres.

  1. Write hh in the form Rcos⁡(θ−α)R\cos(\theta - \alpha).
  2. State the greatest height the water reaches.
  3. Explain why the greatest height is not 12+5=1712 + 5 = 17 m.

You should now be able to

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