Animated Solution for Mathematics - Definite Integration: If ϕ(x)=x1∫π/4x(42sint−3ϕ′(t))dt,x>0, then ϕ′(π/4) is equal to :
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Visualized Solution
Analyze the Given Equation
Given: ϕ(x)=x1∫π/4x(42sint−3ϕ′(t))dt
Objective: Find ϕ′(4π)
Simplify the Equation
Multiply both sides by x to avoid the Quotient Rule.
xϕ(x)=∫π/4x(42sint−3ϕ′(t))dt
Prepare for Differentiation
Differentiate both sides with respect to x.
LHS requires the Product Rule: dxd[u⋅v]=u′v+uv′
RHS requires the Newton-Leibniz Rule: dxd∫axf(t)dt=f(x)
Differentiate the Left Hand Side
Apply Product Rule to xϕ(x):
dxd(xϕ(x))=2x1ϕ(x)+xϕ′(x)
Differentiate the Right Hand Side
Apply Newton-Leibniz Rule to the integral:
dxd∫π/4x(42sint−3ϕ′(t))dt=42sinx−3ϕ′(x)
Equate the Derivatives
Combine the differentiated LHS and RHS:
2xϕ(x)+xϕ′(x)=42sinx−3ϕ′(x)
Find the Boundary Condition ϕ(4π)
Use the original equation: ϕ(x)=x1∫π/4x(42sint−3ϕ′(t))dt
Substitute x=4π:
ϕ(4π)=π/41∫π/4π/4(...)dt
Since upper and lower limits are equal, the integral is 0.
Therefore, ϕ(4π)=0
Substitute x=4π into the Differential Equation
Substitute x=4π and ϕ(4π)=0 into our master equation:
2π/40+4πϕ′(4π)=42sin(4π)−3ϕ′(4π)
Evaluate Trigonometric and Root Terms
Simplify the known values:
sin(4π)=21
4π=2π
The equation becomes: 2πϕ′(4π)=42(21)−3ϕ′(4π)
Simplifying the right side: 2πϕ′(4π)=4−3ϕ′(4π)
Group the ϕ′(4π) Terms
Move all ϕ′(4π) terms to the left side:
2πϕ′(4π)+3ϕ′(4π)=4
Factor out ϕ′(4π):
ϕ′(4π)(2π+3)=4
Simplify the Bracket and Final Calculation
Simplify the expression in the parenthesis:
2π+3=2π+6
The equation becomes: ϕ′(4π)(26+π)=4
Isolate ϕ′(4π):
ϕ′(4π)=6+π4×2=6+π8
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The Sigma Insight: Newton-Leibniz & Reduction Formulas
The Symphony of Calculus
Solving the Integral Equation
Welcome, future engineers! Today, we are going to dissect a problem that perfectly captures the elegance of JEE Advanced mathematics. It is not just about crunching numbers; it is about seeing the structure of the equation and choosing the most graceful path to the solution.
Phase 1
The Algebraic Setup
We are given the equation:
ϕ(x)=x1∫π/4x(42sint−3ϕ′(t))dt
At first glance, it looks intimidating. We have a function ϕ(x) defined by an integral, and we need to find its derivative at a specific point, ϕ′(π/4).
The immediate instinct for many students is to jump straight into differentiation. But stop! If you differentiate immediately, you will be forced to use the Quotient Rule on the right-hand side, which will lead to a messy expression involving x in the denominator.
Instead, let us be strategic. We multiply both sides by x to obtain:
xϕ(x)=∫π/4x(42sint−3ϕ′(t))dt
Now, the equation is linear and clean. This simple algebraic maneuver is the difference between a chaotic calculation and a smooth derivation.
Phase 2
The Calculus Symphony
Now that we have cleared the denominator, we are ready to differentiate both sides with respect to x. On the left-hand side, we have a product of two functions: x and ϕ(x).
We apply the Product Rule:
dxd(xϕ(x))=2x1ϕ(x)+xϕ′(x)
On the right-hand side, we invoke the powerful Newton-Leibniz Rule. This rule is a bridge between integration and differentiation, stating that the derivative of an integral with a variable upper limit x is simply the integrand evaluated at x.
Thus, the right-hand side becomes: 42sinx−3ϕ′(x). Equating the two sides, we get our master differential equation:
2xϕ(x)+xϕ′(x)=42sinx−3ϕ′(x)
Phase 3
The Boundary Condition
We are almost there, but we have a problem. We need to find ϕ′(π/4), but our equation contains ϕ(x). If we plug in x=π/4 right now, we will need the value of ϕ(π/4).
We return to the original integral equation:
ϕ(x)=x1∫π/4x(42sint−3ϕ′(t))dt
If we substitute x=π/4, the integral becomes ∫π/4π/4...dt. By the fundamental properties of definite integrals, an integral from a point to itself is always zero. Therefore, ϕ(π/4)=0.
This is our 'Aha!' moment. The term ϕ(x) vanishes at our point of interest!
Phase 4
The Final Tally
With ϕ(π/4)=0, our master equation at x=π/4 simplifies beautifully:
0+4πϕ′(4π)=42sin(4π)−3ϕ′(4π)
We know that sin(π/4)=1/2 and π/4=π/2. Substituting these values, we get:
2πϕ′(4π)=4−3ϕ′(4π)
Now, it is just simple algebra. Group the ϕ′(π/4) terms:
ϕ′(4π)(2π+3)=4
Simplifying the bracket gives us (π+6)/2. Finally, isolating ϕ′(π/4), we arrive at the final answer:
ϕ′(4π)=6+π8
And there you have it! By staying calm, simplifying the algebra first, and using the Newton-Leibniz rule effectively, we turned a complex problem into a series of elegant steps. Keep practicing, and remember: every problem is just a story waiting to be solved.