Animated Solution for Mathematics - Definite Integration: Let f be a non-negative function defined on the interval [0, 1]. If ∫0x1−(f′(t))2dt=∫0xf(t)dt, 0≤x≤1, and f(0)=0, then
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Visualized Solution
The Integral Equation
Given: ∫0x1−(f′(t))2dt=∫0xf(t)dt
Interval: 0≤x≤1
Initial Condition: f(0)=0
Differentiating the Equation
Apply Newton-Leibniz Rule to differentiate both sides with respect to x.
dxd[∫0x1−(f′(t))2dt]=dxd[∫0xf(t)dt]
Simplifying the Integrals
1−(f′(x))2=f(x)
Squaring Both Sides
Squaring both sides to remove the radical:
1−(f′(x))2=(f(x))2
Rearranging Terms
Rearranging to isolate (f′(x))2:
(f′(x))2=1−(f(x))2
Finding f′(x)
f′(x)=±1−(f(x))2
Since f(x)≥0 and f(0)=0, we take the positive root:
dxdf=1−f2
Setting up the Differential Equation
Separating variables f and x:
1−f2df=dx
Integrating Both Sides
∫1−f2df=∫dx
sin−1(f(x))=x+C
Applying Initial Conditions
Using f(0)=0:
sin−1(0)=0+C
C=0
Revealing f(x)
Substituting C=0:
sin−1(f(x))=x
f(x)=sinx
Comparing sinx and x
For x>0, it is a known property that sinx<x.
Let's visualize this on a graph.
Checking the First Point
At x=21:
f(21)=sin(21)
Since sinx<x, f(21)<21
Checking the Second Point
At x=31:
f(31)=sin(31)
Similarly, f(31)<31
Selecting the Correct Option
Both conditions are satisfied:
f(21)<21 and f(31)<31
This matches Option 3.
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The Sigma Insight: Newton-Leibniz & Reduction Formulas
Solution Diagram
Analyzing the Setup
Welcome, future engineer. Today, we are not just solving a problem; we are embarking on a mathematical detective story. We are given an integral equation:
∫0x1−(f′(t))2dt=∫0xf(t)dt
At first glance, this looks like a formidable wall of symbols. But remember, in the world of JEE Advanced, complexity is often just a mask for elegance. Our first task is to strip away this mask.
The Newton-Leibniz Magic
Whenever you see variable limits in an integral, the Newton-Leibniz rule is your best friend. It is the key that unlocks the door.
By applying dxd to both sides, we effectively differentiate the integral with respect to its upper limit. The integral signs vanish, leaving us with the core relationship:
1−(f′(x))2=f(x)
This is the moment of clarity. We have successfully moved from the realm of integral calculus into the domain of differential equations.
The Birth of a Differential Equation
Now, the problem transforms. We have a radical equation, which can be cumbersome. To make things easier to handle, let's get rid of that square root.
Squaring both sides gives us 1−(f′(x))2=(f(x))2. With a little algebraic rearrangement, we isolate the derivative term:
(f′(x))2=1−(f(x))2
This is beautiful. It is a classic separable differential equation. Since the problem states that f is a non-negative function starting at f(0)=0, the function must be increasing initially. Therefore, we take the positive root:
dxdf=1−f2
The Trigonometric Revelation
We are now in the home stretch. We rearrange the equation to separate the variables:
1−f2df=dx
Integrating both sides is a standard procedure. The integral on the left is the derivative of the inverse sine function, yielding:
sin−1(f(x))=x+C
To find the constant C, we use our initial condition f(0)=0. Plugging this in, we get sin−1(0)=0+C, which means C=0. Substituting C back into our equation, we get sin−1(f(x))=x, or simply:
f(x)=sinx
The Final Verdict
Finally, we compare sinx and x. For any x>0, the sine curve lies strictly below the line y=x. This is a fundamental geometric property.
Therefore, at x=1/2, we have f(1/2)=sin(1/2)<1/2. Similarly, at x=1/3, we have f(1/3)=sin(1/3)<1/3.
Both conditions are satisfied, leading us directly to the correct option. You have conquered the problem, not by brute force, but by peeling back the layers of calculus to reveal the elegant truth beneath.