Given:
\[ \sec^2 x \frac{dx}{dy} + e^{2y} \tan^2 x + \tan x = 0 \]
Step 1: Substitute \( \tan x \) with \( t \).
Let \( t = \tan x \). Then, \( \frac{dt}{dy} = \sec^2 x \frac{dx}{dy} \).
The equation becomes: \[ \frac{dt}{dy} + e^{2y} t^2 + t = 0 \] Rearranging gives: \[ \frac{dt}{dy} + t = -t^2 e^{2y} \]
Step 2: Divide by \( t^2 \).
\[ \frac{1}{t^2} \frac{dt}{dy} + \frac{1}{t} = -e^{2y} \]
Step 3: Substitute \( \frac{1}{t} \) with \( u \).
Let \( u = \frac{1}{t} = t^{-1} \). Then, \( \frac{du}{dy} = -t^{-2} \frac{dt}{dy} = -\frac{1}{t^2} \frac{dt}{dy} \).
The equation transforms to: \[ -\frac{du}{dy} + u = -e^{2y} \] Multiplying by -1 yields: \[ \frac{du}{dy} - u = e^{2y} \]
Step 4: Solve the linear differential equation.
The integrating factor (I.F.) is: \[ e^{\int -1 \, dy} = e^{-y} \]
Multiply the equation by the I.F.: \[ u e^{-y} = \int e^{-y} \times e^{2y} dy \]
Integrating the right side: \[ u e^{-y} = e^{y} + c \]
Step 5: Substitute back for \( u \).
Replace \( u \) with \( \frac{1}{t} \) and \( t \) with \( \tan x \): \[ \frac{1}{\tan x} \times e^{-y} = e^{y} + c \]
Step 6: Apply the given conditions.
Given \( x = \frac{\pi}{4} \) and \( y = 0 \): \[ \frac{1}{\tan(\pi/4)} e^{-0} = e^{0} + c \Rightarrow 1 \times 1 = 1 + c \Rightarrow c = 0 \]
Given \( x = \frac{\pi}{6} \) and \( y = \alpha \). With \( c = 0 \), the equation becomes: \[ \frac{1}{\tan(\pi/6)} e^{-\alpha} = e^{\alpha} \] \[ \frac{1}{1/\sqrt{3}} e^{-\alpha} = e^{\alpha} \Rightarrow \sqrt{3} e^{-\alpha} = e^{\alpha} \] Rearranging the terms: \[ e^{2\alpha} = \sqrt{3} \] Raising both sides to the power of 4: \[ (e^{2\alpha})^4 = (\sqrt{3})^4 \] \[ e^{8\alpha} = 9 \]
Final Answer:
\[ e^{8\alpha} = 9 \]