曲线 C 的参数方程为 x=et,  y=sin⁡tx = e^{t},\ \ y = \sin t 其中 0≤t≤π0 \le t \le \pi。

  1. (i)

    求 ∫etsin⁡t dt\int e^{t}\sin t\,dt。

  2. (ii)

    画出 C 的图形草图。

  3. (iii)

    求由 C、x 轴以及直线 x=1x = 1 和 x=eax = e^{a}(其中 aa 是正实数常数)所围成区域的面积,结果用 aa 表示。

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完整解法

6(i)

1. Apply integration by parts to the given integral.

Let I=∫etsin⁡t dtI = \int e^t \sin t \, dt.

Using the integration by parts formula ∫udvdt dt=uv−∫vdudt dt\int u \frac{dv}{dt} \, dt = uv - \int v \frac{du}{dt} \, dt:
Let u=sin⁡t  ⟹  dudt=cos⁡tu = \sin t \implies \frac{du}{dt} = \cos t
Let dvdt=et  ⟹  v=et\frac{dv}{dt} = e^t \implies v = e^t

I=etsin⁡t−∫etcos⁡t dtI = e^t \sin t - \int e^t \cos t \, dt

2. Apply integration by parts a second time to the new integral.

For ∫etcos⁡t dt\int e^t \cos t \, dt:
Let u=cos⁡t  ⟹  dudt=−sin⁡tu = \cos t \implies \frac{du}{dt} = -\sin t
Let dvdt=et  ⟹  v=et\frac{dv}{dt} = e^t \implies v = e^t

∫etcos⁡t dt=etcos⁡t−∫et(−sin⁡t) dt\int e^t \cos t \, dt = e^t \cos t - \int e^t (-\sin t) \, dt
∫etcos⁡t dt=etcos⁡t+∫etsin⁡t dt\int e^t \cos t \, dt = e^t \cos t + \int e^t \sin t \, dt

3. Substitute the result back and solve algebraically for the original integral $I$.

Substitute the result from the second integration by parts back into the equation for II:
I=etsin⁡t−(etcos⁡t+∫etsin⁡t dt)I = e^t \sin t - \left( e^t \cos t + \int e^t \sin t \, dt \right)
I=etsin⁡t−etcos⁡t−II = e^t \sin t - e^t \cos t - I

Rearranging to solve for II:
2I=et(sin⁡t−cos⁡t)2I = e^t (\sin t - \cos t)
I=12et(sin⁡t−cos⁡t)+CI = \frac{1}{2}e^t (\sin t - \cos t) + C

答案

12et(sin⁡t−cos⁡t)+C\frac{1}{2}e^t(\sin t - \cos t) + C

6(ii)

1. Find the coordinates of the endpoints by substituting the boundary values of $t$.

When t=0t = 0:
x=e0=1x = e^0 = 1
y=sin⁡0=0y = \sin 0 = 0
Start point is (1,0)(1, 0).

When t=πt = \pi:
x=eπx = e^{\pi}
y=sin⁡π=0y = \sin \pi = 0
End point is (eπ,0)(e^{\pi}, 0).

2. Find the coordinates of the maximum point.

The maximum value of y=sin⁡ty = \sin t for 0≤t≤π0 \le t \le \pi occurs at t=π2t = \frac{\pi}{2}, where y=1y = 1.
When t=π2t = \frac{\pi}{2}:
x=eπ/2x = e^{\pi/2}
Turning point (maximum) is (eπ/2,1)(e^{\pi/2}, 1).

3. Sketch the curve noting its domain and shape.

Since x=etx = e^t is strictly increasing, the curve progresses continuously from left to right. The sketch is a bell-like curve in the positive x,yx, y quadrant, starting at (1,0)(1,0), peaking at (eπ/2,1)(e^{\pi/2}, 1), and returning to the x-axis at (eπ,0)(e^{\pi}, 0). The curve is skewed such that the peak is horizontally closer to the starting point.

答案

A smooth curve in the first quadrant starting at (1,0)(1, 0), rising to a maximum point at (eπ/2,1)(e^{\pi/2}, 1), and falling to an end point at (eπ,0)(e^{\pi}, 0). The curve is skewed leftwards.

6(iii)

1. Determine the limits for the parameter $t$ and set up the parametric integral for the area.

When x=1x = 1, et=1  ⟹  t=0e^t = 1 \implies t = 0.
When x=eax = e^a, et=ea  ⟹  t=ae^t = e^a \implies t = a.

The area is given by ∫x=1x=eay dx\int_{x=1}^{x=e^a} y \, dx.
Using x=et  ⟹  dxdt=etx = e^t \implies \frac{dx}{dt} = e^t:
Area=∫t=0t=ay(dxdt)dt=∫0asin⁡t (et) dt\text{Area} = \int_{t=0}^{t=a} y \left(\frac{dx}{dt}\right) dt = \int_{0}^{a} \sin t \, (e^t) \, dt

2. Find the antiderivative $\int e^t \sin t \, dt$ (concisely re-deriving the result required from part (i)).

Let I=∫etsin⁡t dtI = \int e^t \sin t \, dt.
Using integration by parts (u=sin⁡tu = \sin t, dv=et dtdv = e^t \, dt):
I=etsin⁡t−∫etcos⁡t dtI = e^t \sin t - \int e^t \cos t \, dt
Applying integration by parts again on the second integral (u=cos⁡tu = \cos t, dv=et dtdv = e^t \, dt):
I=etsin⁡t−(etcos⁡t−∫et(−sin⁡t) dt)I = e^t \sin t - \left( e^t \cos t - \int e^t (-\sin t) \, dt \right)
I=etsin⁡t−etcos⁡t−II = e^t \sin t - e^t \cos t - I
2I=et(sin⁡t−cos⁡t)2I = e^t(\sin t - \cos t)
∫etsin⁡t dt=12et(sin⁡t−cos⁡t)\int e^t \sin t \, dt = \frac{1}{2} e^t (\sin t - \cos t)

3. Evaluate the definite integral to find the area in terms of $a$.

Area=[12et(sin⁡t−cos⁡t)]0a\text{Area} = \left[ \frac{1}{2} e^t (\sin t - \cos t) \right]_0^a
=12ea(sin⁡a−cos⁡a)−12e0(sin⁡0−cos⁡0)= \frac{1}{2} e^a (\sin a - \cos a) - \frac{1}{2} e^0 (\sin 0 - \cos 0)
=12ea(sin⁡a−cos⁡a)−12(1)(0−1)= \frac{1}{2} e^a (\sin a - \cos a) - \frac{1}{2}(1)(0 - 1)
=12ea(sin⁡a−cos⁡a)+12= \frac{1}{2} e^a (\sin a - \cos a) + \frac{1}{2}

答案

12ea(sin⁡a−cos⁡a)+12\frac{1}{2} e^a (\sin a - \cos a) + \frac{1}{2}

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