Example 6 Express the signal x(t) as Fourier series. Express the Fourier seri...
May 9, 2024
Solution by Steps
step 1
To find the Fourier series coefficients of the given function x(t)=1+sin(ω0t)+2cos(ω0t)+cos(2ω0t+4π), we will use the Fourier series formula for periodic functions
step 2
The Fourier series of a function x(t) is given by a0+∑n=1∞[ancos(nω0t)+bnsin(nω0t)], where a0 is the average value of the function, an are the cosine coefficients, and bn are the sine coefficients
step 3
The coefficient a0 is the average value of the function over one period, which is a0=1 since the constant term in x(t) is 1
step 4
The coefficient a1 corresponds to the cosine term with the fundamental frequency ω0, which is a1=2 due to the term 2cos(ω0t)
step 5
The coefficient b1 corresponds to the sine term with the fundamental frequency ω0, which is b1=1 due to the term sin(ω0t)
step 6
The term cos(2ω0t+4π) can be expanded using the cosine of a sum formula: cos(A+B)=cos(A)cos(B)−sin(A)sin(B)
step 7
Applying the formula from step 6, we get cos(2ω0t+4π)=cos(2ω0t)cos(4π)−sin(2ω0t)sin(4π)
step 8
Since cos(4π)=sin(4π)=22, the term becomes 22cos(2ω0t)−22sin(2ω0t)
step 9
The coefficient a2 is the amplitude of the cosine term with frequency 2ω0, which is a2=22
step 10
The coefficient b2 is the amplitude of the sine term with frequency 2ω0, which is b2=−22
step 11
The Fourier series for x(t) is therefore x(t)=1+2cos(ω0t)+sin(ω0t)+22cos(2ω0t)−22sin(2ω0t)
step 12
To express the coefficients in polar form, we convert each rectangular coefficient pair (an,bn) to polar form using rn=an2+bn2 and θn=arctan(anbn)
step 13
For n=1, we have r1=22+12=5 and θ1=arctan(21)
step 14
For n=2, we have r2=(22)2+(−22)2=21 and θ2=arctan(22−22)=arctan(−1)=−4π
Answer
The Fourier series for x(t) is x(t)=1+2cos(ω0t)+sin(ω0t)+22cos(2ω0t)−22sin(2ω0t). The coefficients in polar form are r1=5, θ1=arctan(21), r2=21, and θ2=−4π.
Key Concept
Fourier Series Coefficients
Explanation
The Fourier series coefficients for a function can be found by identifying the amplitudes of the sine and cosine terms at different frequencies. These coefficients can be expressed in rectangular form as (an,bn) and converted to polar form with magnitude rn and phase θn.