Key Concepts and Formulas
- Substitution Method for Definite Integrals: This technique is used to simplify integrals by changing the variable of integration. It is essential to update the limits of integration according to the substitution.
- Properties of Definite Integrals: Specifically, the property ∫abf(x)dx=−∫baf(x)dx is used to reverse the limits of integration, and the property ∫−aaf(x)dx=∫−aaf(−x)dx is useful for integrals with symmetric limits.
- Algebraic Simplification: Basic algebraic manipulation of exponents and fractions is required.
Step-by-Step Solution
Step 1: Analyze the Integral and Apply Substitution
The given integral is:
I=0∫π(1+cos2x)(ecosx+e−cosx)ecosxsinxdx
We observe that the numerator contains sinxdx, and the terms in the integrand are functions of cosx. This suggests using the substitution t=cosx.
Let t=cosx.
Differentiating both sides with respect to x, we get dxdt=−sinx, which implies dt=−sinxdx, or sinxdx=−dt.
Now, we must change the limits of integration:
When x=0, t=cos(0)=1.
When x=π, t=cos(π)=−1.
Substituting these into the integral, we get:
I=1∫−1(1+t2)(et+e−t)et(−dt)
I=−1∫−1(1+t2)(et+e−t)etdt
Using the property ∫abf(x)dx=−∫baf(x)dx, we can swap the limits of integration and remove the negative sign:
I=−1∫1(1+t2)(et+e−t)etdt... (Equation 1)
Step 2: Apply the Property of Definite Integrals for Symmetric Limits
The integral in Equation 1 has symmetric limits from −1 to 1. We can use the property ∫−aaf(t)dt=∫−aaf(−t)dt.
Let f(t)=(1+t2)(et+e−t)et.
Then, f(−t)=(1+(−t)2)(e−t+e−(−t))e−t=(1+t2)(e−t+et)e−t.
Therefore, we can also write the integral I as:
I=−1∫1(1+t2)(e−t+et)e−tdt... (Equation 2)
Step 3: Combine the Two Forms of the Integral
Now, we add Equation 1 and Equation 2:
I+I=−1∫1(1+t2)(et+e−t)etdt+−1∫1(1+t2)(e−t+et)e−tdt
2I=−1∫1((1+t2)(et+e−t)et+(1+t2)(e−t+et)e−t)dt
Since the denominators are the same, we can combine the numerators:
2I=−1∫1(1+t2)(et+e−t)et+e−tdt
Notice that the term (et+e−t) appears in both the numerator and the denominator. We can cancel this term, provided et+e−t=0, which is always true for real t.
2I=−1∫1(1+t2)1dt
Step 4: Evaluate the Simplified Integral
The integral is now a standard form:
2I=−1∫11+t21dt
The antiderivative of 1+t21 is tan−1(t).
2I=[tan−1(t)]−11
Now, we evaluate the definite integral using the limits:
2I=tan−1(1)−tan−1(−1)
We know that tan−1(1)=4π and tan−1(−1)=−4π.
2I=4π−(−4π)
2I=4π+4π
2I=42π
2I=2π
Step 5: Solve for I
Finally, we solve for I by dividing by 2:
I=21×2π
I=4π
Common Mistakes & Tips
- Forgetting to change limits: When using substitution in definite integrals, always update the limits of integration to correspond to the new variable.
- Sign errors with substitution: The derivative of cosx is −sinx, so remember to include the negative sign when performing the substitution dt=−sinxdx.
- Misapplying the symmetric limit property: Ensure the integrand is indeed an even function of the variable t when using ∫−aaf(t)dt=∫−aaf(−t)dt or an odd function for ∫−aaf(t)dt=0. In this case, we used the property to get an alternative form of the integral and then added them.
Summary
The problem is solved by first applying a trigonometric substitution to simplify the integrand and transform the limits of integration. The resulting integral has symmetric limits, allowing us to use a property of definite integrals to obtain a second form of the integral. By adding the original and transformed integrals, the expression simplifies significantly. The final step involves evaluating a standard integral of 1+t21 and solving for the value of the original integral.
The final answer is 4π.