求证:2−sec⁡2θsec⁡θ(sin⁡θ+cos⁡θ)=1−tan⁡θ\frac{2 - \sec^2 \theta}{\sec \theta (\sin \theta + \cos \theta)} = 1 - \tan \theta。 由此解方程 4−2sec⁡2θsec⁡θ(sin⁡θ+cos⁡θ)=sec⁡2θ−2\frac{4 - 2\sec^2 \theta}{\sec \theta (\sin \theta + \cos \theta)} = \sec^2 \theta - 2,其中 0≤θ≤2π0 \le \theta \le 2\pi。

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完整解法

5(i)

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

LHS=2−1cos⁡2θ1cos⁡θ(sin⁡θ+cos⁡θ)\text{LHS} = \frac{2 - \frac{1}{\cos^2 \theta}}{\frac{1}{\cos \theta} (\sin \theta + \cos \theta)}

2. Simplify the complex fraction by multiplying the numerator and denominator by $\cos^2 \theta$.

LHS=(2−1cos⁡2θ)cos⁡2θ1cos⁡θ(sin⁡θ+cos⁡θ)cos⁡2θ=2cos⁡2θ−1cos⁡θ(sin⁡θ+cos⁡θ)\text{LHS} = \frac{\left(2 - \frac{1}{\cos^2 \theta}\right) \cos^2 \theta}{\frac{1}{\cos \theta} (\sin \theta + \cos \theta) \cos^2 \theta} = \frac{2\cos^2 \theta - 1}{\cos \theta (\sin \theta + \cos \theta)}

3. Use trigonometric identities to rewrite the numerator as a difference of squares.

Since cos⁡2θ=2cos⁡2θ−1=cos⁡2θ−sin⁡2θ\cos 2\theta = 2\cos^2 \theta - 1 = \cos^2 \theta - \sin^2 \theta,

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

4. Factorise the numerator, cancel the common factor, and simplify to reach the right-hand side (RHS).

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

=cos⁡θ−sin⁡θcos⁡θ= \frac{\cos \theta - \sin \theta}{\cos \theta}

=cos⁡θcos⁡θ−sin⁡θcos⁡θ= \frac{\cos \theta}{\cos \theta} - \frac{\sin \theta}{\cos \theta}

=1−tan⁡θ=RHS= 1 - \tan \theta = \text{RHS}

答案

Proof completed.

5(ii)

1. Use the result from part (i) to simplify the left-hand side of the equation.

The left-hand side is 2×2−sec⁡2θsec⁡θ(sin⁡θ+cos⁡θ)2 \times \frac{2 - \sec^2 \theta}{\sec \theta (\sin \theta + \cos \theta)}.
Using (i), LHS =2(1−tan⁡θ)= 2(1 - \tan \theta).

2. Express the right-hand side in terms of $\tan \theta$.

RHS =sec⁡2θ−2= \sec^2 \theta - 2
Since sec⁡2θ=1+tan⁡2θ\sec^2 \theta = 1 + \tan^2 \theta,
RHS =(1+tan⁡2θ)−2=tan⁡2θ−1= (1 + \tan^2 \theta) - 2 = \tan^2 \theta - 1.

3. Form and solve the quadratic equation in $\tan \theta$.

2(1−tan⁡θ)=tan⁡2θ−12(1 - \tan \theta) = \tan^2 \theta - 1
2−2tan⁡θ=tan⁡2θ−12 - 2\tan \theta = \tan^2 \theta - 1
tan⁡2θ+2tan⁡θ−3=0\tan^2 \theta + 2\tan \theta - 3 = 0
(tan⁡θ−1)(tan⁡θ+3)=0(\tan \theta - 1)(\tan \theta + 3) = 0
tan⁡θ=1ortan⁡θ=−3\tan \theta = 1 \quad \text{or} \quad \tan \theta = -3

4. Solve for $\theta$ when $\tan \theta = 1$.

For tan⁡θ=1\tan \theta = 1 in 0≤θ≤2π0 \le \theta \le 2\pi:
θ=π4,π+π4\theta = \frac{\pi}{4}, \pi + \frac{\pi}{4}
θ=π4,5π4\theta = \frac{\pi}{4}, \frac{5\pi}{4}

5. Solve for $\theta$ when $\tan \theta = -3$.

For tan⁡θ=−3\tan \theta = -3 in 0≤θ≤2π0 \le \theta \le 2\pi:
Basic angle α=tan⁡−1(3)≈1.2490\alpha = \tan^{-1}(3) \approx 1.2490
θ\theta is in the 2nd and 4th quadrants.
θ=π−1.2490≈1.89\theta = \pi - 1.2490 \approx 1.89
θ=2π−1.2490≈5.03\theta = 2\pi - 1.2490 \approx 5.03

答案

θ=π4,1.89,5π4,5.03\theta = \frac{\pi}{4}, 1.89, \frac{5\pi}{4}, 5.03

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