Animated Solution for Mathematics - Indefinite Integration: Let f(t)=∫(1−cos(loget)1−sin(loget))dt,t>1. If f(eπ/2)=−eπ/2 and f(eπ/4)=αeπ/4, then α equals
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Visualized Solution
Substitution u=loget
Given integral: f(t)=∫(1−cos(loget)1−sin(loget))dt
Let u=loget⟹t=eu
Differentiating: dt=eudu
Rewriting the Integral
Substituting u and dt:
f(t)=∫eu(1−cosu1−sinu)du
Simplifying the Denominator
Using half-angle identity:
1−cosu=2sin2(2u)
Expanding the Numerator
Using half-angle identity:
sinu=2sin(2u)cos(2u)
Numerator becomes: 1−2sin(2u)cos(2u)
Splitting the Fraction
2sin2(2u)1−2sin(2u)cos(2u)
=2sin2(2u)1−2sin2(2u)2sin(2u)cos(2u)
=21csc2(2u)−cot(2u)
Identifying the Special Integral Form
Current integral: ∫eu[−cot(2u)+21csc2(2u)]du
Recognizing the form: ∫ex[f(x)+f′(x)]dx=exf(x)+C
Verifying the Derivative
Let g(u)=−cot(2u)
Differentiating: g′(u)=−[−csc2(2u)⋅21]
g′(u)=21csc2(2u)
Evaluating the Integral
Integral result: eug(u)+C
=−eucot(2u)+C
Substitute u=loget and eu=t:
f(t)=−tcot(2loget)+C
Applying the First Boundary Condition
Given: f(e2π)=−e2π
Substitute t=e2π into f(t):
f(e2π)=−e2πcot(2loge(e2π))+C
=−e2πcot(22π)+C
Solving for the Constant C
Since cot(4π)=1:
−e2π(1)+C=−e2π
C=0
Final Function: f(t)=−tcot(2loget)
Setting up the Second Condition
Given: f(e4π)=αe4π
Substitute t=e4π into f(t):
f(e4π)=−e4πcot(2loge(e4π))
=−e4πcot(24π)=−e4πcot(8π)
Evaluating cot(8π)
Using the identity: cotθ=sin2θ1+cos2θ
For θ=8π: cot(8π)=sin(4π)1+cos(4π)
=211+21=2+1
Finding the Final Value of α
Comparing both sides: αe4π=−e4πcot(8π)
Cancel e4π: α=−cot(8π)
Substitute the value: α=−(2+1)
Final Answer: α=−1−2
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The Sigma Insight: Evaluation of Special Integral Forms
The Art of Unmasking the Integral
Welcome, future engineer. Today, we are going to dismantle a problem that, at first glance, looks like a chaotic mess of logarithms and trigonometry.
You might feel a shiver of hesitation when you see f(t)=∫(1−cos(loget)1−sin(loget))dt. That is perfectly normal.
In the JEE Advanced arena, the most intimidating problems are often just simple concepts wearing a scary mask. Our job is to strip away that mask.
Phase 1
The Substitution Strategy
The presence of loget inside the trigonometric functions is a massive red flag. It is the 'noise' preventing us from using standard identities.
We need to simplify the domain. Let us perform the substitution u=loget.
This implies t=eu, and consequently, dt=eudu. Suddenly, the integral transforms into:
f(t)=∫eu(1−cosu1−sinu)du
Look at that! We have moved from a logarithmic nightmare to a clean, exponential-trigonometric structure. This is the first victory.
Phase 2
Trigonometric Surgery
Now, we must operate on the fraction 1−cosu1−sinu. In calculus, whenever you see 1−cosu or 1+cosu, your brain should immediately trigger the half-angle identities.
We know that 1−cosu=2sin2(u/2). Similarly, to maintain consistency, we expand sinu as 2sin(u/2)cos(u/2).
Substituting these into our fraction, we get:
2sin2(u/2)1−2sin(u/2)cos(u/2)
By splitting this into two terms, we get 21csc2(u/2)−cot(u/2). This simplifies the expression beautifully.
Phase 3
The Golden Form
We are now looking at the integral ∫eu[−cot(u/2)+21csc2(u/2)]du. Does this look familiar? It should!
This is the legendary ∫ex[f(x)+f′(x)]dx=exf(x)+C pattern. If we define f(u)=−cot(u/2), then its derivative f′(u) is indeed 21csc2(u/2).
The integral collapses instantly into −eucot(u/2)+C. Replacing u with loget, we get:
f(t)=−tcot(2loget)+C
Phase 4
Finding the Constants and the Final Answer
We are given f(eπ/2)=−eπ/2. Substituting this into our result, we find that C=0.
This simplifies our function to f(t)=−tcot(2loget). Finally, we evaluate f(eπ/4)=αeπ/4.
This leads us to α=−cot(π/8). Using the identity cot(π/8)=2+1, we arrive at our final answer:
α=−1−2
See? The monster was just a puzzle waiting to be solved. Keep this logic in your toolkit, and no integral will ever scare you again.