Animated Solution for Mathematics - Differential Equations: If y=y(x) is the solution of the differential equation (1+e2x)dxdy+2(1+y2)ex=0 and y(0)=0, then 6[y′(0)+(y(loge3))2] is equal to:
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Visualized Solution
Identifying the Differential Equation
Given Differential Equation: (1+e2x)dxdy+2(1+y2)ex=0
Initial Condition: y(0)=0
Goal: Find the value of 6[y′(0)+(y(loge3))2]
Variable Separation
Rearranging the terms: (1+e2x)dxdy=−2(1+y2)ex
Separating variables y and x: 1+y2dy=−1+e2x2exdx
Integrating Both Sides
Integrating: ∫1+y2dy=−2∫1+(ex)2exdx
Using the standard formula: ∫1+u21du=tan−1u
Result: tan−1y=−2tan−1(ex)+C
Finding the Constant C
Apply initial condition y(0)=0:
tan−1(0)=−2tan−1(e0)+C
0=−2tan−1(1)+C
0=−2(4π)+C⇒C=2π
The Particular Solution
Substituting C=2π back into the equation:
tan−1y=2π−2tan−1(ex)
Calculating y′(0)
From the original equation: (1+e2x)y′+2(1+y2)ex=0
Substitute x=0,y=0:
(1+e0)y′(0)+2(1+02)e0=0
2y′(0)+2=0⇒y′(0)=−1
Evaluating y at x=loge3
At x=loge3, we have ex=3
Substitute into the particular solution:
tan−1y=2π−2tan−1(3)
tan−1y=2π−2(3π)=2π−32π
tan−1y=−6π⇒y=tan(−6π)=−31
Final Computation
Expression to evaluate: 6[y′(0)+(y(loge3))2]
Substitute y′(0)=−1 and y=−31:
=6[−1+(−31)2]
=6[−1+31]=6[−32]=−4
Final Answer: -4
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The Sigma Insight: Variable Separable Method
Analyzing the Setup
Welcome, fellow traveler of the mathematical landscape. Today, we stand before a problem that might look like a tangled mess of exponentials and derivatives, but it is a beautifully choreographed dance.
When you first look at the equation (1+e2x)dxdy+2(1+y2)ex=0, it is natural to feel a moment of hesitation. Remember, in the world of JEE Advanced, complexity is often just a mask for elegance.
The Art of Separation
Our first mission is to bring order to chaos by isolating our variables. By rearranging the terms, we arrive at the following separation:
1+y2dy=−1+e2x2exdx
Look at the left side—it is the classic derivative of tan−1(y). On the right side, we observe ex in the numerator and (ex)2 in the denominator.
This is a perfect setup for a substitution. If we let u=ex, then du=exdx. The integral becomes a standard form, and the path forward clears.
Finding the Constant of Truth
Integrating both sides, we obtain:
tan−1y=−2tan−1(ex)+C
This C is our constant of integration, the signature of our specific curve. We are given the initial condition y(0)=0.
Plugging these values in, we find 0=−2tan−1(1)+C. Since tan−1(1)=4π, we find that C=2π. Our particular solution is now locked in:
tan−1y=2π−2tan−1(ex)
The Final Calculation
We need to evaluate 6[y′(0)+(y(loge3))2]. We do not need to differentiate the entire function to find y′(0).
Simply return to the original differential equation and substitute x=0 and y=0. This yields 2y′(0)+2=0, which gives us y′(0)=−1.
Next, we tackle y(loge3). Substituting x=loge3 into our particular solution, we get ex=3.
Thus, tan−1y=2π−2tan−1(3). Since tan−1(3)=3π, we have tan−1y=2π−32π=−6π. Therefore, y=tan(−6π)=−31.
The Grand Finale
We are at the finish line. We have y′(0)=−1 and y=−31. Plugging these into our expression:
6[−1+(−31)2]=6[−1+31]=6[−32]=−4
The final result is -4. We started with a daunting differential equation, navigated through integration, applied initial conditions, and arrived at a clean, integer result. This is the beauty of mathematics—the logic holds, the steps align, and the truth reveals itself.