Animated Solution for Mathematics - Definite Integration: The value of the integral ∫−ln2ln2ex(ln(ex+1+e2x))dx is equal to
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Visualized Solution
Analyze the Integral
Given Integral: I=∫−ln2ln2exln(ex+1+e2x)dx
Observe the structure: The term ex is present both as a factor and within the argument of the logarithm.
Substitution Method
Let ex=t
Differentiating both sides: exdx=dt
Changing the Limits
Lower limit: When x=−ln2, t=e−ln2=21
Upper limit: When x=ln2, t=eln2=2
Rewriting the Integral
Substituting t and dt into the integral:
I=∫212ln(t+1+t2)dt
Integration by Parts Setup
Using Integration by Parts: ∫udv=uv−∫vdu
Let u=ln(t+1+t2) and dv=dt
Then v=t
Differentiating the Log Term
Find du using Chain Rule:
du=t+1+t21⋅(1+21+t22t)dt
du=t+1+t21⋅(1+t21+t2+t)dt=1+t21dt
Applying the IBP Formula
Applying IBP formula:
I=[tln(t+1+t2)]212−∫2121+t2tdt
Integrating the Second Term
Evaluate ∫1+t2tdt:
Let 1+t2=z⟹2tdt=dz
∫2z1dz=z=1+t2
Combining the Results
Combining both parts of the integral:
I=[tln(t+1+t2)−1+t2]212
Evaluating at Upper Limit
At t=2:
Value =2ln(2+22+1)−22+1
Value =2ln(2+5)−5
Evaluating at Lower Limit
At t=21:
Value =21ln(21+1+41)−1+41
Value =21ln(21+5)−25
Subtracting the Limits
Subtracting the values: I=(2ln(2+5)−5)−(21ln(21+5)−25)
I=2ln(2+5)−21ln(21+5)−25
Final Simplification
I=ln((2+5)2)−ln(21+5)−25
I=ln(1+52(2+5)2)−25
Final Answer:ln(1+52(2+5)2)−25
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The Sigma Insight: Fundamental Theorem & Properties of Definite Integrals
Solution Diagram
Analyzing the Setup
The given integral is:
I=∫−ln2ln2exln(ex+1+e2x)dx
At first glance, this expression appears to be a daunting, tangled mess of exponentials and logarithms. However, in the context of JEE Advanced, appearances are often deceiving. The key to unlocking this problem lies in recognizing the hidden symmetry.
Notice how ex appears both as a factor and inside the logarithm. This is a classic invitation to use the substitution method. By setting t=ex, we transform the variable x into t, and the differential exdx becomes dt.
The Transformation
When we perform the substitution t=ex, we must also update our limits of integration. When x=−ln2, t=e−ln2=21. When x=ln2, t=eln2=2.
Our integral now becomes:
I=∫212ln(t+1+t2)dt
This is a much cleaner, more elegant form. We are now looking for the area under the curve of the natural log of t plus the square root of 1+t2.
The Art of Integration by Parts
To tackle the integral of a lone logarithmic function, we turn to our most powerful tool: Integration by Parts. We set u=ln(t+1+t2) and dv=dt, which implies v=t.
The magic happens when we calculate du. Using the chain rule, the derivative of ln(t+1+t2) is:
du=t+1+t21⋅(1+21+t22t)dt
Simplifying this, we get:
du=t+1+t21⋅1+t21+t2+tdt=1+t21dt
The complexity vanishes!
The Grand Finale
Applying the Integration by Parts formula, I=[uv]−∫vdu, we obtain:
I=[tln(t+1+t2)]212−∫2121+t2tdt
The second integral is a standard form, resulting in 1+t2. Combining everything, we have:
I=[tln(t+1+t2)−1+t2]212
Evaluating at the upper limit t=2 and the lower limit t=21, we calculate: