Prove the identity cot⁡θ−1=cos⁡2θsin⁡θ(cos⁡θ+sin⁡θ)\cot \theta - 1 = \dfrac{\cos 2\theta}{\sin \theta (\cos \theta + \sin \theta)}. Hence solve the equation cos⁡4θsin⁡2θ(cos⁡2θ+sin⁡2θ)=−12\dfrac{\cos 4\theta}{\sin 2\theta(\cos 2\theta + \sin 2\theta)} = -\dfrac{1}{2} for −180∘≤θ≤180∘-180^\circ \le \theta \le 180^\circ.

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Worked solution

11(a)

1. Apply the double angle formula for cosine to the numerator of the right-hand side.

RHS=cos⁡2θsin⁡θ(cos⁡θ+sin⁡θ)\text{RHS} = \frac{\cos 2\theta}{\sin \theta (\cos \theta + \sin \theta)}
=cos⁡2θ−sin⁡2θsin⁡θ(cos⁡θ+sin⁡θ)= \frac{\cos^2 \theta - \sin^2 \theta}{\sin \theta (\cos \theta + \sin \theta)}

2. Factorise the numerator using the difference of two squares and cancel the common factor.

=(cos⁡θ−sin⁡θ)(cos⁡θ+sin⁡θ)sin⁡θ(cos⁡θ+sin⁡θ)= \frac{(\cos \theta - \sin \theta)(\cos \theta + \sin \theta)}{\sin \theta (\cos \theta + \sin \theta)}
=cos⁡θ−sin⁡θsin⁡θ= \frac{\cos \theta - \sin \theta}{\sin \theta}

3. Split the fraction and use the definition of cotangent to reach the left-hand side.

=cos⁡θsin⁡θ−sin⁡θsin⁡θ= \frac{\cos \theta}{\sin \theta} - \frac{\sin \theta}{\sin \theta}
=cot⁡θ−1= \cot \theta - 1
=LHS (proven)= \text{LHS (proven)}

Answer

Proof completed.

11(b)

1. Apply the identity from part (a) to simplify the equation

From part (a), we have cot⁡α−1=cos⁡2αsin⁡α(cos⁡α+sin⁡α)\cot \alpha - 1 = \dfrac{\cos 2\alpha}{\sin \alpha (\cos \alpha + \sin \alpha)}.
Letting α=2θ\alpha = 2\theta, the equation becomes:
cot⁡2θ−1=−12\cot 2\theta - 1 = -\dfrac{1}{2}

2. Rearrange to find $\tan 2\theta$

cot⁡2θ=12\cot 2\theta = \dfrac{1}{2}
tan⁡2θ=2\tan 2\theta = 2

3. Determine the basic angle and the range for $2\theta$

Basic angle α=tan⁡−1(2)≈63.435∘\alpha = \tan^{-1}(2) \approx 63.435^\circ
Given −180∘≤θ≤180∘-180^\circ \le \theta \le 180^\circ, the range for 2θ2\theta is −360∘≤2θ≤360∘-360^\circ \le 2\theta \le 360^\circ.

4. Find all possible values for $2\theta$ in the required range

Since tan⁡2θ>0\tan 2\theta > 0, 2θ2\theta lies in the 1st and 3rd quadrants.
2θ=63.435∘,63.435∘+180∘,63.435∘−180∘,63.435∘−360∘2\theta = 63.435^\circ, 63.435^\circ + 180^\circ, 63.435^\circ - 180^\circ, 63.435^\circ - 360^\circ
2θ=63.435∘,243.435∘,−116.565∘,−296.565∘2\theta = 63.435^\circ, 243.435^\circ, -116.565^\circ, -296.565^\circ

5. Solve for $\theta$ and round to 1 decimal place

θ=31.717∘,121.717∘,−58.282∘,−148.282∘\theta = 31.717^\circ, 121.717^\circ, -58.282^\circ, -148.282^\circ
θ=−148.3∘,−58.3∘,31.7∘,121.7∘\theta = -148.3^\circ, -58.3^\circ, 31.7^\circ, 121.7^\circ (to 1 d.p.)

Answer

θ=−148.3∘,−58.3∘,31.7∘,121.7∘\theta = -148.3^\circ, -58.3^\circ, 31.7^\circ, 121.7^\circ

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