Finding Exponential Fourier Series for a Periodic Signal

Click For Summary
SUMMARY

The discussion focuses on finding the exponential Fourier series for the periodic signal defined as x(t) = 2 + (1/2)cos(t + 45°) + 2cos(3t) - 2sin(4t + 30°). The correct fundamental frequency is determined to be ω₀ = 1 rad/s, derived from the least common multiple of the periods 2π/3, 2π, and π/2. The conversion of cosine and sine terms to their exponential forms using Euler's formula is confirmed, with the sine term correctly transformed to fit the exponential representation.

PREREQUISITES
  • Understanding of Fourier series and periodic signals
  • Familiarity with Euler's formula and complex exponentials
  • Knowledge of trigonometric identities and transformations
  • Ability to calculate least common multiples of periods
NEXT STEPS
  • Study the derivation of Fourier series for different types of periodic signals
  • Learn about the application of Euler's formula in signal processing
  • Explore the relationship between sine and cosine functions in complex exponential forms
  • Investigate the implications of fundamental frequency in signal analysis
USEFUL FOR

Students and professionals in electrical engineering, signal processing, and applied mathematics who are working with Fourier analysis and periodic signals.

VinnyCee
Messages
486
Reaction score
0

Homework Statement



For the periodic signal

x(t)\,=\,2\,+\,\frac{1}{2}\,cos\left(t\,+\,45^{\circ}\right)\,+\,2\,cos\left(3\,t\right)\,-\,2\,sin\left(4\,t\,+\,30^{\circ}\right)

Find the exponential Fourier series.

Homework Equations



Euler’s Formula
x(t)\,=\,A\,cos\left(\omega_0\,t\,+\,\phi\right)\,=\,A\,\left[e^{j\,\left(\omega_0\,t\,+\,\phi\right)}\,+\, e^{-j\,\left(\omega_0\,t\,+\,\phi\right)}\right]

The Attempt at a Solution



To get \omega_0, we need to find the least common denominator between the following periods…

\frac{2\,\pi}{3},\,2\,\pi,\,\frac{\pi}{2}

Which is 2\,\pi.So, now I use the formula \omega_0\,=\,\frac{2\,\pi}{T}…

\omega_0\,=\,\frac{2\,\pi}{2\,\pi}\,=\,1Now, I use Euler’s formula to convert the cos and sin to exponentials…

x(t)\,=\,2\,+\,\frac{1}{2}\,\left[e^{j\left(t\,+\,45^{\circ}\right)}\,+\,e^{-j\left(t\,+\,45^{\circ}\right)\right]\,+\,2\,\left[e^{j\left(3\,t\right)}\,+\,e^{-j\left(3\,t\right)}\right]\,-\,2\left[e^{j\left(4\,t\,-\,60^{\circ}\right)}\,+\,e^{-j\left(4\,t\,-\,60^{\circ}\right)}\right]

I don’t know if the last term (sin) is supposed to be kept as 4\,t\,+\,30^{\circ}

OR changed to a cosine to fit Euler’s formula by subtracting ninety degrees: 4\,t\,-\,60^{\circ}I assumed the latter, is that correct?
 
Physics news on Phys.org
VinnyCee said:
To get \omega_0, we need to find the least common denominator between the following periods…

\frac{2\,\pi}{3},\,2\,\pi,\,\frac{\pi}{2}

Which is 2\,\pi.

So, now I use the formula \omega_0\,=\,\frac{2\,\pi}{T}…

\omega_0\,=\,\frac{2\,\pi}{2\,\pi}\,=\,1
I think you meant "least common multiple."

Anyway, your approach seems unnecessarily complicated. Other than the constant term, the Fourier series has terms of the form ##\cos n\omega_0 t## and ##\sin n\omega_0 t##. You can see, by inspection, that ##\omega_0=1~\rm rad/s## for the signal you were given.

VinnyCee said:
Now, I use Euler’s formula to convert the cos and sin to exponentials…
x(t)=2+\frac 12 \left[e^{j(t+45^\circ)}+e^{-j(t+45^\circ)}\right]+2\left[e^{j(3t)}+e^{-j(3t)}\right]-2\left[e^{j(4t-60^\circ)}+e^{-j(4t-60^\circ)}\right]I don’t know if the last term (sin) is supposed to be kept as ##4t+30^\circ## OR changed to a cosine to fit Euler’s formula by subtracting ninety degrees: ##4t-60^\circ##. I assumed the latter. Is that correct?
Yes, that's correct.

Alternatively, you could use the expression for sine in terms of complex exponentials:
$$\sin \theta = \frac{e^{j\theta}-e^{-j\theta}}{2j}.$$
 

Similar threads

Replies
1
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 16 ·
Replies
16
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 8 ·
Replies
8
Views
3K
  • · Replies 5 ·
Replies
5
Views
2K
Replies
2
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K