使用分部积分法(或其它方法),求 ∫1yln⁡y dy\displaystyle\int \frac{1}{y}\ln y\,dy。 已知 y>1y>1 且 dydx=yln⁡y\displaystyle\frac{dy}{dx}=\frac{y}{\ln y},求用 xx 表示 yy 的表达式。 证明 ddx[xsin⁡(ln⁡x)−xcos⁡(ln⁡x)]=2sin⁡(ln⁡x)\displaystyle\frac{d}{dx}\big[x\sin(\ln x)-x\cos(\ln x)\big]=2\sin(\ln x)。 求 ∫e1/2e2/2∣sin⁡(ln⁡x)∣ dx\displaystyle\int_{e^{1/2}}^{e^{2/2}}\big|\sin(\ln x)\big|\,dx 的精确值。

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完整解法

10(a)(i)

1. Define a suitable substitution for the integral.

Let u=ln⁡yu = \ln y.
Then dudy=1y  ⟹  du=1y dy\frac{du}{dy} = \frac{1}{y} \implies du = \frac{1}{y} \,dy.

2. Transform the integral entirely into terms of $u$.

∫1yln⁡y dy=∫u du\int \frac{1}{y} \ln y \,dy = \int u \,du

3. Integrate with respect to $u$, then substitute back $y$ and add the constant of integration.

∫u du=12u2+C\int u \,du = \frac{1}{2}u^2 + C
=12(ln⁡y)2+C= \frac{1}{2}(\ln y)^2 + C

答案

12(ln⁡y)2+C\displaystyle\frac{1}{2}(\ln y)^2 + C

10(a)(ii)

1. Evaluate the integral from part (a)(i) to use in this part.

To find ∫1yln⁡y dy\displaystyle\int \frac{1}{y}\ln y\,dy:
Let u=ln⁡yu = \ln y, then du=1ydydu = \frac{1}{y}dy.
∫u du=12u2=12(ln⁡y)2\displaystyle\int u\,du = \frac{1}{2}u^2 = \frac{1}{2}(\ln y)^2.

2. Separate the variables of the differential equation and integrate.

dydx=yln⁡y\displaystyle\frac{dy}{dx} = \frac{y}{\ln y}
∫ln⁡yy dy=∫1 dx\displaystyle\int \frac{\ln y}{y} \,dy = \int 1 \,dx
Using the result from (a)(i):
12(ln⁡y)2=x+C\displaystyle\frac{1}{2}(\ln y)^2 = x + C, where CC is an arbitrary constant.

3. Make $y$ the subject, using the condition $y>1$ to determine the correct sign of the square root.

(ln⁡y)2=2x+2C(\ln y)^2 = 2x + 2C
ln⁡y=±2x+2C\ln y = \pm\sqrt{2x + 2C}
Since it is given that y>1y > 1, we know ln⁡y>0\ln y > 0. Thus, we must reject the negative root.
ln⁡y=2x+2C\ln y = \sqrt{2x + 2C}
y=e2x+2Cy = e^{\sqrt{2x + 2C}}
Letting c=2Cc = 2C, the general solution is y=e2x+cy = e^{\sqrt{2x + c}}.

答案

y=e2x+cy = e^{\sqrt{2x + c}}

10(b)(i)

1. Apply the product rule and chain rule to differentiate both terms

ddx[xsin⁡(ln⁡x)−xcos⁡(ln⁡x)]=[1⋅sin⁡(ln⁡x)+x⋅cos⁡(ln⁡x)⋅1x]−[1⋅cos⁡(ln⁡x)+x⋅(−sin⁡(ln⁡x))⋅1x]\begin{aligned} \frac{d}{dx}\big[x\sin(\ln x)-x\cos(\ln x)\big] &= \left[ 1 \cdot \sin(\ln x) + x \cdot \cos(\ln x) \cdot \frac{1}{x} \right] - \left[ 1 \cdot \cos(\ln x) + x \cdot (-\sin(\ln x)) \cdot \frac{1}{x} \right] \end{aligned}

2. Simplify the resulting expression to show the required result

ddx[xsin⁡(ln⁡x)−xcos⁡(ln⁡x)]=(sin⁡(ln⁡x)+cos⁡(ln⁡x))−(cos⁡(ln⁡x)−sin⁡(ln⁡x))=sin⁡(ln⁡x)+cos⁡(ln⁡x)−cos⁡(ln⁡x)+sin⁡(ln⁡x)=2sin⁡(ln⁡x)\begin{aligned} \frac{d}{dx}\big[x\sin(\ln x)-x\cos(\ln x)\big] &= \big(\sin(\ln x) + \cos(\ln x)\big) - \big(\cos(\ln x) - \sin(\ln x)\big) \\ &= \sin(\ln x) + \cos(\ln x) - \cos(\ln x) + \sin(\ln x) \\ &= 2\sin(\ln x) \end{aligned}

答案

2sin⁡(ln⁡x)\displaystyle 2\sin(\ln x) (Shown)

10(b)(ii)

1. Determine the sign of $\sin(\ln x)$ on the interval $[e^{1/2}, e^{2/2}]$ to resolve the absolute value.

For x∈[e1/2,e2/2]x \in [e^{1/2}, e^{2/2}] (which simplifies to [e0.5,e][e^{0.5}, e]), the bounds for ln⁡x\ln x are:
12≤ln⁡x≤1\frac{1}{2} \le \ln x \le 1
Since 0<12≤ln⁡x≤1<π0 < \frac{1}{2} \le \ln x \le 1 < \pi, we know that sin⁡(ln⁡x)>0\sin(\ln x) > 0 strictly within this interval.
Thus, the absolute value can be dropped:
∣sin⁡(ln⁡x)∣=sin⁡(ln⁡x)\big|\sin(\ln x)\big| = \sin(\ln x)

2. Apply the given derivative from part (b)(i) to find the antiderivative of $\sin(\ln x)$.

From part (b)(i), we are given:
ddx[xsin⁡(ln⁡x)−xcos⁡(ln⁡x)]=2sin⁡(ln⁡x)\frac{d}{dx}\big[x\sin(\ln x)-x\cos(\ln x)\big]=2\sin(\ln x)
Integrating both sides with respect to xx gives:
∫sin⁡(ln⁡x) dx=12[xsin⁡(ln⁡x)−xcos⁡(ln⁡x)]+C\int \sin(\ln x)\,dx = \frac{1}{2}\big[x\sin(\ln x)-x\cos(\ln x)\big] + C

3. Evaluate the definite integral using the limits.

∫e1/2e2/2∣sin⁡(ln⁡x)∣ dx=∫e1/2esin⁡(ln⁡x) dx\int_{e^{1/2}}^{e^{2/2}}\big|\sin(\ln x)\big|\,dx = \int_{e^{1/2}}^{e} \sin(\ln x)\,dx
=[12(xsin⁡(ln⁡x)−xcos⁡(ln⁡x))]e1/2e= \left[ \frac{1}{2}\big(x\sin(\ln x)-x\cos(\ln x)\big) \right]_{e^{1/2}}^{e}
Substitute x=ex = e and x=e1/2x = e^{1/2}:
=12(esin⁡(1)−ecos⁡(1))−12(e1/2sin⁡(12)−e1/2cos⁡(12))= \frac{1}{2}\big(e\sin(1)-e\cos(1)\big) - \frac{1}{2}\big(e^{1/2}\sin(\tfrac{1}{2})-e^{1/2}\cos(\tfrac{1}{2})\big)
=e2(sin⁡1−cos⁡1)−e2(sin⁡0.5−cos⁡0.5)= \frac{e}{2}(\sin 1 - \cos 1) - \frac{\sqrt{e}}{2}(\sin 0.5 - \cos 0.5)

答案

e2(sin⁡1−cos⁡1)−e2(sin⁡0.5−cos⁡0.5)\frac{e}{2}(\sin 1 - \cos 1) - \frac{\sqrt{e}}{2}(\sin 0.5 - \cos 0.5)

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