变量 xx 和 yy 满足微分方程 πdydx+y(3−πtan⁡x)=0\pi \dfrac{dy}{dx} + y(3 - \pi \tan x) = 0。

  1. (a)

    通过代换 y=zsec⁡xy = z\sec x,证明 dzdx=−3zπ\dfrac{dz}{dx} = -\dfrac{3z}{\pi}。由此证明,满足当 x=π3x = \dfrac{\pi}{3} 时 y=2y = 2 的特解可以表示为 ycos⁡x=ea+bxy\cos x = e^{a+bx} 的形式,其中 aa 和 bb 是待求常数。

  2. (b)

    对于在 (a) 部分中求得的解的图像,求最靠近 yy 轴的两条垂直渐近线的方程。

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完整解法

3(a)

1. Differentiate the given substitution with respect to $x$.

Using the product rule on y=zsec⁡xy = z\sec x:
dydx=dzdxsec⁡x+zsec⁡xtan⁡x\frac{dy}{dx} = \frac{dz}{dx}\sec x + z\sec x \tan x

2. Substitute $y$ and $\frac{dy}{dx}$ into the given differential equation.

Substitute into πdydx+y(3−πtan⁡x)=0\pi \frac{dy}{dx} + y(3 - \pi \tan x) = 0:
π(dzdxsec⁡x+zsec⁡xtan⁡x)+(zsec⁡x)(3−πtan⁡x)=0\pi \left( \frac{dz}{dx}\sec x + z\sec x \tan x \right) + (z\sec x)(3 - \pi \tan x) = 0

3. Expand and simplify to obtain the given expression for $\frac{dz}{dx}$.

πsec⁡xdzdx+πzsec⁡xtan⁡x+3zsec⁡x−πzsec⁡xtan⁡x=0\pi \sec x \frac{dz}{dx} + \pi z\sec x \tan x + 3z\sec x - \pi z\sec x \tan x = 0
πsec⁡xdzdx+3zsec⁡x=0\pi \sec x \frac{dz}{dx} + 3z\sec x = 0
Dividing by πsec⁡x\pi \sec x (since sec⁡x≠0\sec x \neq 0):
dzdx+3zπ=0\frac{dz}{dx} + \frac{3z}{\pi} = 0
dzdx=−3zπ\frac{dz}{dx} = -\frac{3z}{\pi}

4. Separate the variables and integrate.

∫1z dz=∫−3π dx\int \frac{1}{z} \,dz = \int -\frac{3}{\pi} \,dx
ln⁡z=−3πx+C\ln z = -\frac{3}{\pi}x + C

5. Substitute back $z = y\cos x$ and apply the initial conditions to find the constant $C$.

Since y=zsec⁡xy = z\sec x, we have z=ycos⁡xz = y\cos x.
ln⁡(ycos⁡x)=−3πx+C\ln (y\cos x) = -\frac{3}{\pi}x + C
Substitute x=π3x = \frac{\pi}{3} and y=2y = 2:
ln⁡(2cos⁡π3)=−3π(π3)+C\ln \left(2\cos\frac{\pi}{3}\right) = -\frac{3}{\pi}\left(\frac{\pi}{3}\right) + C
ln⁡(2⋅12)=−1+C\ln \left(2 \cdot \frac{1}{2}\right) = -1 + C
ln⁡1=−1+C  ⟹  C=1\ln 1 = -1 + C \implies C = 1

6. Express the solution in the required exponential form and identify constants $a$ and $b$.

Substitute C=1C = 1 back into the equation:
ln⁡(ycos⁡x)=1−3πx\ln (y\cos x) = 1 - \frac{3}{\pi}x
ycos⁡x=e1−3πxy\cos x = e^{1 - \frac{3}{\pi}x}
Comparing with ycos⁡x=ea+bxy\cos x = e^{a+bx}, we have:
a=1,  b=−3πa = 1, \; b = -\frac{3}{\pi}

答案

ycos⁡x=e1−3πxy\cos x = e^{1 - \frac{3}{\pi}x}
a=1,  b=−3πa = 1, \; b = -\frac{3}{\pi}

3(b)

1. Identify the condition for vertical asymptotes from the solution's equation.

From part (a), the solution can be rewritten as y=ea+bxcos⁡xy = \frac{e^{a+bx}}{\cos x}.

Vertical asymptotes occur where the denominator approaches zero while the numerator remains non-zero. Since ea+bx>0e^{a+bx} > 0 for all real xx, the vertical asymptotes correspond exactly to the roots of:
cos⁡x=0\cos x = 0

2. Solve for the two asymptotes closest to the y-axis.

Solving cos⁡x=0\cos x = 0 gives:
x=±π2,±3π2,±5π2,…x = \pm \frac{\pi}{2}, \pm \frac{3\pi}{2}, \pm \frac{5\pi}{2}, \dots

The two vertical asymptotes with equations closest to the yy-axis (x=0x=0) are:
x=π2andx=−π2x = \frac{\pi}{2} \quad \text{and} \quad x = -\frac{\pi}{2}

答案

x=π2x = \frac{\pi}{2} and x=−π2x = -\frac{\pi}{2}

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