The variables xx and yy are related by the differential equation πdydx+y(3−πtan⁡x)=0\pi \dfrac{dy}{dx} + y(3 - \pi \tan x) = 0.

  1. (a)

    Using the substitution y=zsec⁡xy = z\sec x, show that dzdx=−3zπ\dfrac{dz}{dx} = -\dfrac{3z}{\pi}. Hence, show that the particular solution for which y=2y = 2 when x=π3x = \dfrac{\pi}{3} can be expressed in the form ycos⁡x=ea+bxy\cos x = e^{a+bx} where aa and bb are constants to be determined.

  2. (b)

    For the graph of the solution found in part (a), find the equations of the two vertical asymptotes closest to the y-axis.

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Worked solution

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}

Answer

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}

Answer

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

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