The equation provided is:
an=12∫−11f(t)cos(nt)dt=∫−10(t+1)cos(nt)dt+∫01(−t+1)cos(nt)dt
Let's solve each integral step by step.
Step 1: Evaluate the first integral
The first integral is:
∫−10(t+1)cos(nt)dt
We will use integration by parts to solve this integral. Let:
- u=t+1, hence du=dt
- dv=cos(nt)dt, hence v=nsin(nt)
Using integration by parts, ∫udv=uv−∫vdu, we get:
∫(t+1)cos(nt)dt=(t+1)nsin(nt)−∫nsin(nt)dt
The integral of sin(nt) is:
∫sin(nt)dt=−ncos(nt)
Thus:
∫−10(t+1)cos(nt)dt=[n(t+1)sin(nt)+n2cos(nt)]−10
Now, evaluate from −1 to 0:
At t=0:
n(0+1)sin(0)+n2cos(0)=0+n21=n21
At t=−1:
n(−1+1)sin(−n)+n2cos(−n)=0+n2cos(n)=n2cos(n)
So, the first integral evaluates to:
n21−n2cos(n)=n21−cos(n)
Step 2: Evaluate the second integral
The second integral is:
∫01(−t+1)cos(nt)dt
Similarly, using integration by parts:
- u=−t+1, du=−dt
- dv=cos(nt)dt, v=nsin(nt)
Thus:
∫(−t+1)cos(nt)dt=(−t+1)nsin(nt)−∫nsin(nt)(−dt)
This simplifies to:
∫01(−t+1)cos(nt)dt=[n(−t+1)sin(nt)−n2cos(nt)]01
Now, evaluate from 0 to 1:
At t=1:
n(−1+1)sin(n)−n2cos(n)=0−n2cos(n)=−n2cos(n)
At t=0:
n(0−1)sin(0)−n2cos(0)=0−n21=−n21
So, the second integral evaluates to:
−n2cos(n)+n21=n21−cos(n)
Step 3: Combine the results
Now, summing the results of the two integrals:
an=n21−cos(n)+n21−cos(n)=n22(1−cos(n))
So the final answer is:
an=n22(1−cos(n))
Would you like further clarification or details on any of these steps?
Here are some related questions to further explore:
- How does the result change if n is a specific integer value, like n=1 or n=2?
- What happens if the cosine function is replaced with a sine function in the integrals?
- How can we apply this method to different piecewise functions?
- What is the physical interpretation of an in the context of Fourier series?
- How does the Fourier series change if the function f(t) has different boundary conditions?
Tip: When dealing with trigonometric integrals, integration by parts is a powerful tool, especially when the product of a polynomial and a trigonometric function is involved.