Prove the identity tan⁡A−cot⁡Atan⁡A+cot⁡A=1−2cos⁡2A\dfrac{\tan A - \cot A}{\tan A + \cot A} = 1 - 2\cos^{2} A. Hence solve the equation tan⁡2θ−cot⁡2θtan⁡2θ+cot⁡2θ=12\frac{\tan 2\theta - \cot 2\theta}{\tan 2\theta + \cot 2\theta} = \frac{1}{2} for 0<θ<π0 < \theta < \pi, giving your answers in terms of π\pi.

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Worked solution

10(a)

1. Express the left-hand side (LHS) in terms of sine and cosine.

LHS=tan⁡A−cot⁡Atan⁡A+cot⁡A=sin⁡Acos⁡A−cos⁡Asin⁡Asin⁡Acos⁡A+cos⁡Asin⁡A\text{LHS} = \frac{\tan A - \cot A}{\tan A + \cot A} = \frac{\frac{\sin A}{\cos A} - \frac{\cos A}{\sin A}}{\frac{\sin A}{\cos A} + \frac{\cos A}{\sin A}}

2. Simplify the complex fraction by multiplying the numerator and denominator by $\sin A \cos A$.

LHS=sin⁡2A−cos⁡2Asin⁡2A+cos⁡2A\text{LHS} = \frac{\sin^2 A - \cos^2 A}{\sin^2 A + \cos^2 A}

3. Apply the Pythagorean identity to the denominator.

Since sin⁡2A+cos⁡2A=1\sin^2 A + \cos^2 A = 1,
LHS=sin⁡2A−cos⁡2A1=sin⁡2A−cos⁡2A\text{LHS} = \frac{\sin^2 A - \cos^2 A}{1} = \sin^2 A - \cos^2 A

4. Substitute $\sin^2 A = 1 - \cos^2 A$ to obtain the right-hand side (RHS).

LHS=(1−cos⁡2A)−cos⁡2A\text{LHS} = (1 - \cos^2 A) - \cos^2 A
LHS=1−2cos⁡2A=RHS\text{LHS} = 1 - 2\cos^2 A = \text{RHS}

Answer

Proof completed.

10(b)

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

From part (a), tan⁡A−cot⁡Atan⁡A+cot⁡A=1−2cos⁡2A\frac{\tan A - \cot A}{\tan A + \cot A} = 1 - 2\cos^{2} A.
Substituting A=2θA = 2\theta, the equation becomes:
1−2cos⁡2(2θ)=121 - 2\cos^{2}(2\theta) = \frac{1}{2}

2. Rearrange to solve for $\cos^{2}(2\theta)$ and then $\cos(2\theta)$.

2cos⁡2(2θ)=1−12=122\cos^{2}(2\theta) = 1 - \frac{1}{2} = \frac{1}{2}
cos⁡2(2θ)=14\cos^{2}(2\theta) = \frac{1}{4}
cos⁡(2θ)=±12\cos(2\theta) = \pm \frac{1}{2}

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

Given 0<θ<π0 < \theta < \pi, the range for 2θ2\theta is 0<2θ<2π0 < 2\theta < 2\pi.
The basic angle α\alpha for cos⁡α=12\cos \alpha = \frac{1}{2} is π3\frac{\pi}{3}.

4. Find all possible values for $2\theta$ and then $\theta$.

For cos⁡(2θ)=12\cos(2\theta) = \frac{1}{2}:
2θ=π3,2π−π3=5π32\theta = \frac{\pi}{3}, 2\pi - \frac{\pi}{3} = \frac{5\pi}{3}
For cos⁡(2θ)=−12\cos(2\theta) = -\frac{1}{2}:
2θ=π−π3=2π3,π+π3=4π32\theta = \pi - \frac{\pi}{3} = \frac{2\pi}{3}, \pi + \frac{\pi}{3} = \frac{4\pi}{3}
So, 2θ=π3,2π3,4π3,5π32\theta = \frac{\pi}{3}, \frac{2\pi}{3}, \frac{4\pi}{3}, \frac{5\pi}{3}.
Dividing by 2:
θ=π6,π3,2π3,5π6\theta = \frac{\pi}{6}, \frac{\pi}{3}, \frac{2\pi}{3}, \frac{5\pi}{6}

Answer

θ=π6,5π6\theta = \frac{\pi}{6}, \frac{5\pi}{6}

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