曲线 CC 由参数方程定义 x=t−sin⁡tx = t - \sin t,y=sin⁡2ty = \sin^{2} t,  0≤t≤π\;0 \le t \le \pi。 曲线 CC 上的点 AA 对应的参数为 π2\dfrac{\pi}{2},且是一个极大值点。直线 ll 穿过原点和点 AA。区域 RR 由 CC 和 ll 围成,如下图所示。

  1. (i)

    求 AA 的坐标。

  2. (ii)

    使用代数方法,求 RR 的精确面积。

  3. (iii)

    证明 CC 的直角坐标方程为 x=sin⁡−1 ⁣y−yx = \sin^{-1}\!\sqrt{y} - \sqrt{y}。

  4. (iv)

    求当 RR 绕 yy 轴旋转 2π2\pi 弧度时所形成的旋转体的体积。

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完整解法

8(i)

1. Substitute the parameter $t = \frac{\pi}{2}$ into the parametric equations to find the coordinates of $A$.

Given t=π2t = \frac{\pi}{2},
x=π2−sin⁡(π2)=π2−1x = \frac{\pi}{2} - \sin\left(\frac{\pi}{2}\right) = \frac{\pi}{2} - 1
y=sin⁡2(π2)=12=1y = \sin^{2}\left(\frac{\pi}{2}\right) = 1^{2} = 1

The coordinates of AA are (π2−1,1)\left(\frac{\pi}{2} - 1, 1\right).

答案

(π2−1,1)(\frac{\pi}{2} - 1, 1)

8(ii)

1. Find the exact coordinates of point $A$.

Given that point AA corresponds to parameter t=π2t = \frac{\pi}{2}, we substitute this into the parametric equations:
x=π2−sin⁡(π2)=π2−1x = \frac{\pi}{2} - \sin\left(\frac{\pi}{2}\right) = \frac{\pi}{2} - 1
y=sin⁡2(π2)=1y = \sin^2\left(\frac{\pi}{2}\right) = 1
So, the coordinates of AA are (π2−1,1)\left(\frac{\pi}{2} - 1, 1\right).

2. Set up the parametric integral for the area under the curve $C$.

The area under curve CC from x=0x = 0 to x=π2−1x = \frac{\pi}{2} - 1 is given by ∫y dx\int y \, dx.
Using parametric integration, we substitute yy and dxdt\frac{dx}{dt}:
dxdt=1−cos⁡t\frac{dx}{dt} = 1 - \cos t
Area under C=∫t=0t=π/2ydxdt dt\text{Area under } C = \int_{t=0}^{t=\pi/2} y \frac{dx}{dt} \, dt
=∫0π/2sin⁡2t(1−cos⁡t) dt= \int_{0}^{\pi/2} \sin^2 t (1 - \cos t) \, dt
=∫0π/2(sin⁡2t−sin⁡2tcos⁡t) dt= \int_{0}^{\pi/2} (\sin^2 t - \sin^2 t \cos t) \, dt

3. Evaluate the exact area under the curve using trigonometric identities and standard integrals.

To integrate sin⁡2t\sin^2 t, we use the double-angle identity: sin⁡2t=1−cos⁡2t2\sin^2 t = \frac{1 - \cos 2t}{2}.
The integral becomes:
Area under C=∫0π/2(12−12cos⁡2t−sin⁡2tcos⁡t) dt\text{Area under } C = \int_{0}^{\pi/2} \left( \frac{1}{2} - \frac{1}{2}\cos 2t - \sin^2 t \cos t \right) \, dt
Integrating term by term gives:
=[12t−14sin⁡2t−13sin⁡3t]0π/2= \left[ \frac{1}{2}t - \frac{1}{4}\sin 2t - \frac{1}{3}\sin^3 t \right]_{0}^{\pi/2}
Substituting the upper limit t=π2t = \frac{\pi}{2}:
12(π2)−14sin⁡(π)−13sin⁡3(π2)=π4−0−13\frac{1}{2}\left(\frac{\pi}{2}\right) - \frac{1}{4}\sin(\pi) - \frac{1}{3}\sin^3\left(\frac{\pi}{2}\right) = \frac{\pi}{4} - 0 - \frac{1}{3}
Substituting the lower limit t=0t = 0 gives 00.
So, Area under C=π4−13\text{Area under } C = \frac{\pi}{4} - \frac{1}{3}.

4. Calculate the area under the line $l$ (a triangle) and find the exact area of $R$.

The area under the line ll forms a right-angled triangle with the xx-axis. Its base is the xx-coordinate of AA and its height is the yy-coordinate of AA.
Area of triangle=12×base×height=12(π2−1)(1)=π4−12\text{Area of triangle} = \frac{1}{2} \times \text{base} \times \text{height} = \frac{1}{2} \left(\frac{\pi}{2} - 1\right) (1) = \frac{\pi}{4} - \frac{1}{2}
The required exact area of RR is the area under CC minus the area of the triangle:
Area of R=(π4−13)−(π4−12)\text{Area of } R = \left( \frac{\pi}{4} - \frac{1}{3} \right) - \left( \frac{\pi}{4} - \frac{1}{2} \right)
=12−13= \frac{1}{2} - \frac{1}{3}
=16= \frac{1}{6}

答案

\frac{1}{6}

8(iii)

1. Express $\sin t$ in terms of $y$, noting the range of $t$ for the relevant portion of the curve.

From y=sin⁡2ty = \sin^{2} t, we have sin⁡t=±y\sin t = \pm\sqrt{y}.
For the portion of the curve from OO to AA (which bounds region RR), the parameter tt lies in the interval 0≤t≤π20 \le t \le \frac{\pi}{2}.
Since sin⁡t≥0\sin t \ge 0 for this interval, we take the positive root:
sin⁡t=y\sin t = \sqrt{y}

2. Express $t$ in terms of $y$ and substitute into the parametric equation for $x$.

Since 0≤t≤π20 \le t \le \frac{\pi}{2}, the principal value of the inverse sine function applies, giving:
t=sin⁡−1 ⁣yt = \sin^{-1}\!\sqrt{y}
Substitute tt and sin⁡t\sin t into the equation for xx:
x=t−sin⁡tx = t - \sin t
x=sin⁡−1 ⁣y−y  (shown)x = \sin^{-1}\!\sqrt{y} - \sqrt{y}\ \text{ (shown)}

答案

x=sin⁡−1 ⁣y−yx = \sin^{-1}\!\sqrt{y} - \sqrt{y}

8(iv)

1. Identify the equation of the line $l$ passing through the origin and point $A$.

The origin is O(0,0)O(0,0) and from part (i), AA has coordinates (π2−1,1)\left(\frac{\pi}{2} - 1, 1\right).
The gradient of line ll with respect to the yy-axis is xy=π2−11\frac{x}{y} = \frac{\frac{\pi}{2} - 1}{1}.
The equation of the line ll is therefore x=(π2−1)yx = \left(\frac{\pi}{2} - 1\right)y.

2. Set up the definite integrals for the volume of revolution about the $y$-axis.

The solid is generated by rotating the region RR about the yy-axis. The volume VV is given by V=π∫01xouter2 dy−π∫01xinner2 dyV = \pi \int_{0}^{1} x_{\text{outer}}^2 \, \mathrm{d}y - \pi \int_{0}^{1} x_{\text{inner}}^2 \, \mathrm{d}y.
From the given coordinates, the line ll forms the outer boundary and the curve CC forms the inner boundary.
Using the Cartesian equation for CC from (iii), x=sin⁡−1 ⁣y−yx = \sin^{-1}\!\sqrt{y} - \sqrt{y}.
V=π∫01[(π2−1)y]2dy−π∫01(sin⁡−1 ⁣y−y)2dyV = \pi \int_{0}^{1} \left[ \left(\frac{\pi}{2} - 1\right)y \right]^2 \mathrm{d}y - \pi \int_{0}^{1} \left( \sin^{-1}\!\sqrt{y} - \sqrt{y} \right)^2 \mathrm{d}y

3. Evaluate the definite integrals using a graphing calculator to find the volume.

Since an exact algebraic evaluation is not explicitly requested, we can directly evaluate the definite integrals using a graphing calculator:
V≈π(0.10860)−π(0.02819)V \approx \pi (0.10860) - \pi (0.02819)
V≈0.25261V \approx 0.25261
V≈0.253 (to 3 s.f.)V \approx 0.253 \text{ (to 3 s.f.)}

答案

0.2530.253 units3^3

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