曲线 CC 的参数方程为
x=2cos⁡θ+cos⁡2θ,y=2sin⁡θ−sin⁡2θ,x = 2\cos\theta + \cos 2\theta, \quad y = 2\sin\theta - \sin 2\theta,
其中 0<θ<2π0 < \theta < 2\pi 且 θ≠2π3,π,4π3\theta \ne \frac{2\pi}{3}, \pi, \frac{4\pi}{3}。
点 PP 的参数为 pp,且点 PP 在曲线 CC 上。直线 MpM_p 和 NpN_p 分别是曲线 CC 在点 PP 处的切线和法线。

  1. (a)

    已知
    sin⁡A+sin⁡B=2sin⁡A+B2cos⁡A−B2且\sin A + \sin B = 2\sin\frac{A+B}{2}\cos\frac{A-B}{2} \quad \text{且}
    cos⁡A−cos⁡B=−2sin⁡A+B2sin⁡A−B2.\cos A - \cos B = -2\sin\frac{A+B}{2}\sin\frac{A-B}{2}.
    利用这两个结果,证明 MpM_p 的斜率是 −tan⁡(p2)-\tan\left(\frac{p}{2}\right)。

  2. (b)

    当 p=π3p = \frac{\pi}{3} 时,MpM_p 和 NpN_p 分别交 xx 轴于点 QQ 和 RR。求 ΔPQR\Delta PQR 的面积。

  3. (c)

    参数为 ss 的点 SS 落在 CC 上,且直线 NsN_s 是 CC 在点 SS 处的法线。已知 MpM_p 和 NsN_s 平行。

    已知 p≠π3,5π3p \ne \frac{\pi}{3}, \frac{5\pi}{3} 且 p<sp < s,利用结果 tan⁡(A−B)=tan⁡A−tan⁡B1+tan⁡Atan⁡B\tan(A-B) = \frac{\tan A - \tan B}{1 + \tan A \tan B},求一个关于 pp 和 ss 的方程。

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完整解法

11(a)

1. Differentiate $x$ with respect to $\theta$ and simplify using the given trigonometric identity.

dxdθ=−2sin⁡θ−2sin⁡2θ\frac{dx}{d\theta} = -2\sin\theta - 2\sin 2\theta
dxdθ=−2(sin⁡2θ+sin⁡θ)\frac{dx}{d\theta} = -2(\sin 2\theta + \sin\theta)
Using sin⁡A+sin⁡B=2sin⁡A+B2cos⁡A−B2\sin A + \sin B = 2\sin\frac{A+B}{2}\cos\frac{A-B}{2} with A=2θA=2\theta and B=θB=\theta:
dxdθ=−2(2sin⁡3θ2cos⁡θ2)=−4sin⁡3θ2cos⁡θ2\frac{dx}{d\theta} = -2 \left( 2\sin\frac{3\theta}{2}\cos\frac{\theta}{2} \right) = -4\sin\frac{3\theta}{2}\cos\frac{\theta}{2}

2. Differentiate $y$ with respect to $\theta$ and simplify using the given trigonometric identity.

dydθ=2cos⁡θ−2cos⁡2θ\frac{dy}{d\theta} = 2\cos\theta - 2\cos 2\theta
dydθ=2(cos⁡θ−cos⁡2θ)\frac{dy}{d\theta} = 2(\cos\theta - \cos 2\theta)
Using cos⁡A−cos⁡B=−2sin⁡A+B2sin⁡A−B2\cos A - \cos B = -2\sin\frac{A+B}{2}\sin\frac{A-B}{2} with A=θA=\theta and B=2θB=2\theta:
dydθ=2(−2sin⁡3θ2sin⁡(−θ2))\frac{dy}{d\theta} = 2 \left( -2\sin\frac{3\theta}{2}\sin\left(-\frac{\theta}{2}\right) \right)
Since sin⁡(−α)=−sin⁡α\sin(-\alpha) = -\sin\alpha:
dydθ=4sin⁡3θ2sin⁡θ2\frac{dy}{d\theta} = 4\sin\frac{3\theta}{2}\sin\frac{\theta}{2}

3. Use the chain rule for parametric equations to find $\frac{dy}{dx}$ and evaluate the gradient at $\theta = p$.

dydx=(dydθ)(dxdθ)\frac{dy}{dx} = \frac{\left( \frac{dy}{d\theta} \right)}{\left( \frac{dx}{d\theta} \right)}
dydx=4sin⁡3θ2sin⁡θ2−4sin⁡3θ2cos⁡θ2\frac{dy}{dx} = \frac{4\sin\frac{3\theta}{2}\sin\frac{\theta}{2}}{-4\sin\frac{3\theta}{2}\cos\frac{\theta}{2}}
dydx=−sin⁡θ2cos⁡θ2=−tan⁡(θ2)\frac{dy}{dx} = -\frac{\sin\frac{\theta}{2}}{\cos\frac{\theta}{2}} = -\tan\left(\frac{\theta}{2}\right)
At point PP, θ=p\theta = p, so the gradient of the tangent MpM_p is −tan⁡(p2)-\tan\left(\frac{p}{2}\right) (shown).

答案

Gradient of Mp=−tan⁡(p2)\text{Gradient of } M_p = -\tan\left(\frac{p}{2}\right)

11(b)

1. Calculate the coordinates of point $P$ at $p = \frac{\pi}{3}$.

xP=2cos⁡(π3)+cos⁡(2π3)=2(12)−12=12x_P = 2\cos\left(\frac{\pi}{3}\right) + \cos\left(\frac{2\pi}{3}\right) = 2\left(\frac{1}{2}\right) - \frac{1}{2} = \frac{1}{2}

yP=2sin⁡(π3)−sin⁡(2π3)=2(32)−32=32y_P = 2\sin\left(\frac{\pi}{3}\right) - \sin\left(\frac{2\pi}{3}\right) = 2\left(\frac{\sqrt{3}}{2}\right) - \frac{\sqrt{3}}{2} = \frac{\sqrt{3}}{2}

So, PP is (12,32)\left(\frac{1}{2}, \frac{\sqrt{3}}{2}\right).

2. Find the gradients of the tangent $M_p$ and normal $N_p$ at $P$.

From part (a), the gradient of the tangent MpM_p is −tan⁡(p2)-\tan\left(\frac{p}{2}\right).
At p=π3p = \frac{\pi}{3}, the gradient of MpM_p is:
mt=−tan⁡(π6)=−13m_t = -\tan\left(\frac{\pi}{6}\right) = -\frac{1}{\sqrt{3}}

Since the normal NpN_p is perpendicular to MpM_p, the gradient of NpN_p is:
mn=−1mt=3m_n = -\frac{1}{m_t} = \sqrt{3}

3. Determine the coordinates of $Q$ and $R$ by finding the $x$-intercepts of $M_p$ and $N_p$.

Equation of MpM_p:
y−32=−13(x−12)y - \frac{\sqrt{3}}{2} = -\frac{1}{\sqrt{3}}\left(x - \frac{1}{2}\right)
To find QQ, substitute y=0y = 0:
−32=−13(x−12)  ⟹  32=x−12  ⟹  x=2-\frac{\sqrt{3}}{2} = -\frac{1}{\sqrt{3}}\left(x - \frac{1}{2}\right) \implies \frac{3}{2} = x - \frac{1}{2} \implies x = 2
So, QQ is (2,0)(2, 0).

Equation of NpN_p:
y−32=3(x−12)y - \frac{\sqrt{3}}{2} = \sqrt{3}\left(x - \frac{1}{2}\right)
To find RR, substitute y=0y = 0:
−32=3(x−12)  ⟹  −12=x−12  ⟹  x=0-\frac{\sqrt{3}}{2} = \sqrt{3}\left(x - \frac{1}{2}\right) \implies -\frac{1}{2} = x - \frac{1}{2} \implies x = 0
So, RR is (0,0)(0, 0).

4. Calculate the area of $\Delta PQR$.

The base QRQR lies on the xx-axis with length 2−0=22 - 0 = 2.
The perpendicular height of ΔPQR\Delta PQR is the yy-coordinate of PP, which is 32\frac{\sqrt{3}}{2}.

Area=12×base×height\text{Area} = \frac{1}{2} \times \text{base} \times \text{height}
Area=12(2)(32)=32\text{Area} = \frac{1}{2}(2)\left(\frac{\sqrt{3}}{2}\right) = \frac{\sqrt{3}}{2}

答案

32\frac{\sqrt{3}}{2}

11(c)

1. Equate the gradients of $M_p$ and $N_s$.

From part (a), the gradient of the tangent at parameter θ\theta is −tan⁡(θ2)-\tan\left(\frac{\theta}{2}\right).

The gradient of the tangent MpM_p at parameter pp is mMp=−tan⁡(p2)m_{M_p} = -\tan\left(\frac{p}{2}\right).

The gradient of the normal NsN_s at parameter ss is mNs=−1−tan⁡(s2)=1tan⁡(s2)m_{N_s} = \frac{-1}{-\tan\left(\frac{s}{2}\right)} = \frac{1}{\tan\left(\frac{s}{2}\right)}.

Since MpM_p and NsN_s are parallel, their gradients are equal:
−tan⁡(p2)=1tan⁡(s2)-\tan\left(\frac{p}{2}\right) = \frac{1}{\tan\left(\frac{s}{2}\right)}
tan⁡(s2)tan⁡(p2)=−1\tan\left(\frac{s}{2}\right) \tan\left(\frac{p}{2}\right) = -1
1+tan⁡(s2)tan⁡(p2)=01 + \tan\left(\frac{s}{2}\right) \tan\left(\frac{p}{2}\right) = 0

2. Apply the given trigonometric identity to find the relationship between $p$ and $s$.

Substitute A=s2A = \frac{s}{2} and B=p2B = \frac{p}{2} into the given identity tan⁡(A−B)=tan⁡A−tan⁡B1+tan⁡Atan⁡B\tan(A-B) = \frac{\tan A - \tan B}{1 + \tan A \tan B}:
tan⁡(s2−p2)=tan⁡(s2)−tan⁡(p2)1+tan⁡(s2)tan⁡(p2)\tan\left(\frac{s}{2} - \frac{p}{2}\right) = \frac{\tan\left(\frac{s}{2}\right) - \tan\left(\frac{p}{2}\right)}{1 + \tan\left(\frac{s}{2}\right) \tan\left(\frac{p}{2}\right)}

Since 1+tan⁡(s2)tan⁡(p2)=01 + \tan\left(\frac{s}{2}\right) \tan\left(\frac{p}{2}\right) = 0, the denominator is zero, meaning tan⁡(s−p2)\tan\left(\frac{s-p}{2}\right) is undefined.

For the tangent function to be undefined, the angle must be π2+kπ\frac{\pi}{2} + k\pi for some integer kk.
Given 0<p<2π0 < p < 2\pi and 0<s<2π0 < s < 2\pi with p<sp < s, we know that 0<s−p<2π0 < s - p < 2\pi, which means 0<s−p2<π0 < \frac{s-p}{2} < \pi.

The only value in this range where tangent is undefined is π2\frac{\pi}{2}.
s−p2=π2\frac{s-p}{2} = \frac{\pi}{2}
s−p=πs - p = \pi

答案

s−p=πs - p = \pi

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