Animated Solution for Mathematics - Differential Equations: Let ∫0x1−(y′(t))2dt=∫0xy(t)dt,0≤x≤3,y≥0,y(0)=0. Then at x=2,y′′+y+1 is equal to
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Visualized Solution
Analyze the Integral Equation
Given equation: ∫0x1−(y′(t))2dt=∫0xy(t)dt
Initial condition: y(0)=0
Constraint: 0≤x≤3,y≥0
Introduce Leibniz Rule
To free y(x) from the integrals, we differentiate both sides with respect to x.
Tool: Newton-Leibniz Rule.
dxd∫0xf(t)dt=f(x)
Apply Leibniz Rule
Differentiating both sides:
dxd∫0x1−(y′(t))2dt=dxd∫0xy(t)dt
Result: 1−(y′(x))2=y(x)
Simplify the Equation
To remove the square root, square both sides:
(1−(y′)2)2=(y)2
1−(y′)2=y2
Isolate the Derivative
Rearrange to isolate (y′)2:
(y′)2=1−y2
Take the square root: y′=1−y2
Variable Separable Form
Rewrite y′ as dxdy:
dxdy=1−y2
Separate the variables y and x:
1−y2dy=dx
Integrate Both Sides
Integrate both sides:
∫1−y2dy=∫dx
Standard integral result:
sin−1(y)=x+C
Find the Constant of Integration
Use the initial condition y(0)=0.
Substitute x=0,y=0:
sin−1(0)=0+C
0=0+C⇒C=0
Determine the Function y(x)
Substitute C=0 back into the equation:
sin−1(y)=x
Take sine of both sides:
y(x)=sin(x)
Calculate Derivatives
We need y′′ for the final expression.
First derivative: y′(x)=dxd(sinx)=cosx
Second derivative: y′′(x)=dxd(cosx)=−sinx
Final Evaluation
Target expression: y′′+y+1
Substitute y=sinx and y′′=−sinx:
(−sinx)+(sinx)+1=1
At x=2, the value remains 1.
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The Sigma Insight: Variable Separable Method
Solution Diagram
Analyzing the Setup
Welcome, fellow traveler on the path to JEE mastery. Today, we are going to dismantle a problem that, at first glance, looks like a fortress.
You have an integral equation:
∫0x1−(y′(t))2dt=∫0xy(t)dt
The unknown function y(t) is trapped behind integral signs on both sides, and we are given the boundary condition y(0)=0. But here is the secret: in mathematics, every cage has a key. Our key today is the Newton-Leibniz Rule.
The Leibniz Key
To free y(x) from these integral cages, we must perform a surgical operation: differentiation. We differentiate both sides with respect to x.
The Newton-Leibniz Rule tells us that the derivative of the integral from zero to x of a function is simply the function evaluated at x. Applying dxd to both sides, the integral signs vanish, leaving us with a much cleaner differential equation:
1−(y′(x))2=y(x)
The Algebraic Dance
Now, look at that square root. To liberate our derivative y′, we square both sides:
1−(y′)2=y2
Rearranging the terms to isolate the derivative, we obtain (y′)2=1−y2. Taking the square root, we arrive at:
y′=1−y2
This is a first-order differential equation, and it is begging to be solved using the method of variable separation.
The Path to Sine
We rewrite y′ as dxdy and separate the variables:
1−y2dy=dx
Integrating both sides, we recall the classic result from your calculus toolkit:
sin−1(y)=x+C
Using our initial condition y(0)=0, we find that C=0. Thus, sin−1(y)=x, which means our mystery function is y(x)=sinx.
The Grand Finale
We have found the function! The question asks for the value of y′′+y+1 at x=2.
First, we differentiate y=sinx twice:
y′=cosx
y′′=−sinx
Now, substitute these into our target expression:
(−sinx)+(sinx)+1
Look at that beautiful cancellation! The sine terms vanish, leaving us with the constant 1.
The value is independent of x, so even at x=2, the final answer is 1. You have conquered the integral, solved the differential equation, and found the hidden constant. Well done!