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Find the general solution of the differe...

Find the general solution of the differential equation: `cos^(2)x(dy)/(dx)+y=tanx`. Find the particular solution which satisfies `y=0` at `x=0`.

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To solve the differential equation \( \cos^2 x \frac{dy}{dx} + y = \tan x \), we will follow these steps: ### Step 1: Rearranging the Equation We start by rewriting the equation in a standard form: \[ \frac{dy}{dx} + \frac{y}{\cos^2 x} = \frac{\tan x}{\cos^2 x} \] This simplifies to: \[ \frac{dy}{dx} + y \sec^2 x = \tan x \sec^2 x \] ### Step 2: Identifying \( p(x) \) and \( q(x) \) Here, we identify: - \( p(x) = \sec^2 x \) - \( q(x) = \tan x \sec^2 x \) ### Step 3: Finding the Integrating Factor The integrating factor \( \mu(x) \) is given by: \[ \mu(x) = e^{\int p(x) \, dx} = e^{\int \sec^2 x \, dx} = e^{\tan x} \] ### Step 4: Multiplying the Equation by the Integrating Factor We multiply the entire differential equation by the integrating factor: \[ e^{\tan x} \frac{dy}{dx} + e^{\tan x} y \sec^2 x = e^{\tan x} \tan x \sec^2 x \] This simplifies to: \[ \frac{d}{dx}(e^{\tan x} y) = e^{\tan x} \tan x \sec^2 x \] ### Step 5: Integrating Both Sides Now we integrate both sides: \[ \int \frac{d}{dx}(e^{\tan x} y) \, dx = \int e^{\tan x} \tan x \sec^2 x \, dx \] The left side simplifies to: \[ e^{\tan x} y = \int e^{\tan x} \tan x \sec^2 x \, dx \] ### Step 6: Solving the Right Side Integral To solve the right side, we can use integration by parts. Let: - \( u = \tan x \) - \( dv = e^{\tan x} \sec^2 x \, dx \) Then, we have: - \( du = \sec^2 x \, dx \) - \( v = e^{\tan x} \) Using integration by parts: \[ \int u \, dv = uv - \int v \, du \] This gives: \[ \int \tan x e^{\tan x} \sec^2 x \, dx = \tan x e^{\tan x} - \int e^{\tan x} \sec^2 x \, dx \] ### Step 7: Final Form of the General Solution After solving the integral, we find: \[ e^{\tan x} y = e^{\tan x} \tan x - e^{\tan x} + C \] Dividing by \( e^{\tan x} \): \[ y = \tan x - 1 + Ce^{-\tan x} \] ### Step 8: Finding the Particular Solution To find the particular solution that satisfies \( y(0) = 0 \): Substituting \( x = 0 \): \[ 0 = \tan(0) - 1 + Ce^{-\tan(0)} \] This simplifies to: \[ 0 = 0 - 1 + C \cdot 1 \implies C = 1 \] ### Final Particular Solution Substituting \( C = 1 \) back into the general solution: \[ y = \tan x - 1 + e^{-\tan x} \] ### Summary The general solution is: \[ y = \tan x - 1 + Ce^{-\tan x} \] The particular solution is: \[ y = \tan x - 1 + e^{-\tan x} \]
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