Industry-relevant training in Business, Technology, and Design to help professionals and graduates upskill for real-world careers.
Fun, engaging games to boost memory, math fluency, typing speed, and English skillsβperfect for learners of all ages.
Listen to a student-teacher conversation explaining the topic in a relatable way.
Signup and Enroll to the course for listening the Audio Lesson
Today, we are discussing an interesting phenomenon related to the Fourier series, particularly when it encounters discontinuous signals. What do you think happens to a signal, like a square wave, when we try to approximate it using Fourier series?
I think there might be some issues since the square wave jumps from one value to another suddenly.
Exactly! When we try to represent a square wave using a finite number of terms in a Fourier series, we can experience whatβs called the Gibbs phenomenon, where we see oscillations at the discontinuities.
Does that mean the approximation looks like itβs 'ringing' around the jump?
Yes! Thatβs a very good observation. The term βringingβ refers to how the approximation overshoots right before the discontinuity and undershoots shortly afterward. This effect becomes more pronounced even as more terms are added.
So the overshoot doesn't disappear? How much does it typically overshoot?
Great question, Student_3! The overshoot is approximately 9% of the magnitude of the jump at the discontinuity. For example, if a square wave jumps from -1 to +1, the overshoot will be around 0.179 units.
Signup and Enroll to the course for listening the Audio Lesson
Now let's explore why this phenomenon occurs. Can anyone explain what happens when we try to represent an instantaneous jump in a signal?
I suppose because the signal changes so quickly, a few sinusoidal functions can't replicate it properly?
Spot on, Student_4! Finite sums of continuous functions, like our sine and cosine, can't capture these abrupt changes perfectly. We technically would need an infinite number of sine waves to achieve that.
But if I keep adding terms, the overshoot should decrease, right?
Not really. While the ringing does narrow down as more terms are added, the overshoot itself remains nearly constant. The spatial width of these oscillations does decrease, but they never entirely go away. At the jump, the approximation converges to the average of the limits on both sides of the discontinuity.
Signup and Enroll to the course for listening the Audio Lesson
Understanding the Gibbs phenomenon is crucial in various applications. Can someone hypothesize where this might pose a problem?
In digital signal processing, maybe? If there's ringing, it might cause artifacts in the sound?
Exactly! Artifacts in audio or visual signals can be problematic. As for mitigation, what do you think we might do to reduce these overshoots?
Perhaps using windowing functions on the coefficients?
Right again! Windowing can smooth out the effects by tapering the Fourier coefficients, which in turn can reduce the overshoot, although it might also affect the sharpness of the reconstructed signal.
So itβs a trade-off between sharpness and ringing!
Exactly, Student_4! Itβs all about finding that balance.
Read a summary of the section's main ideas. Choose from Basic, Medium, or Detailed.
The Gibbs phenomenon refers to the oscillations and overshoot that occur when a finite number of Fourier series terms approximate a discontinuous signal. This section highlights the behavior observed near discontinuities and emphasizes practical implications in various engineering fields.
The section introduces the concept of the Gibbs phenomenon, explaining how Fourier series, while effective for representing periodic signals, struggles with discontinuous inputs like square or sawtooth waves. When such a discontinuous signal is approximated using a finite number of terms from its Fourier series, characteristics known as oscillations or 'ringing' appear near the discontinuities.
Dive deep into the subject with an immersive audiobook experience.
Signup and Enroll to the course for listening the Audio Book
While the Fourier series is remarkably effective at representing a wide range of periodic signals, it exhibits a peculiar characteristic when the signal contains abrupt discontinuities (e.g., sharp jumps, like in a square wave or a saw-tooth wave).
This chunk introduces the main issue addressed in this section: the limitations of the Fourier series when dealing with periodic signals that have abrupt jumps or discontinuities. Typically, Fourier series effectively represent smooth and continuous functions. However, when a signal exhibits sudden changes, such as the sharp transitions of a square wave, the Fourier series struggle to provide an accurate representation. The problem lies in the fact that these discontinuities require infinite frequencies for precise reproduction, which is not achievable with a finite number of terms in a Fourier series.
Think of this issue like trying to draw a sharp corner using a brush; no matter how many strokes you make, the corner will always appear rounded due to the softness of the bristles. Similarly, no matter how many terms you add to the Fourier series, you can't perfectly recreate the sharp jumpβonly approximate it.
Signup and Enroll to the course for listening the Audio Book
When a discontinuous periodic signal is approximated by a finite number of terms (a partial sum) from its Fourier series, oscillations or "ringing" are observed in the vicinity of the discontinuities. More specifically, there's a pronounced overshoot just before the jump and an undershoot just after the jump.
This chunk explains the specific behaviorβcommonly referred to as 'ringing'βthat occurs when approximating discontinuous signals with the Fourier series. When trying to approximate a sharp discontinuity with sinusoidal components, the Fourier series produces oscillations around the points of discontinuity. These oscillations take the form of an overshoot just before the discontinuity and an undershoot afterward, leading to an appearance of spikes or waves at the transition points. This phenomenon is characteristic of the Gibbs phenomenon and demonstrates how well Fourier series can approximate smooth transitions versus how they struggle with abrupt changes.
Imagine watching a movie scene where a light suddenly turns on; if the scene were slowly faded in, youβd hardly notice the change. However, if itβs jumped, you might see flickers or continuity issues as the lighting adjusts, resembling the overshoot and undershoot in the Fourier representation.
Signup and Enroll to the course for listening the Audio Book
Imagine plotting the partial sum of the Fourier series for a square wave. As you add more and more terms, the approximation gets progressively better in the smooth regions of the square wave. However, right at the edges of the square wave (the discontinuities), you will always see these "spikes" or "ears" that overshoot the actual value of the square wave. Even as you add a very large number of terms, these overshoots remain.
This chunk discusses a conceptual visual understanding of how the Gibbs phenomenon manifests when plotting functions approximated by a Fourier series. When you plot the Fourier series approximating a square wave, initially, you see a mismatched representation, especially at the jump edges. As you keep increasing the number of terms in the Fourier series, the approximation improves in smooth areas of the signal but fails to eliminate the distinctive spikes at the discontinuities. These spikes persist regardless of how many terms are included, demonstrating that the Fourier series cannot fully replicate the sharp transitions.
Consider music synthesis; when you layer sounds together, at certain times, you might hear distortions or overtones that overshadow the actual notes. Even adding more layers (terms) doesnβt eliminate that distortionβsimilarly to how more Fourier series terms canβt eliminate the visual spikes in the signal approximation.
Learn essential terms and foundational ideas that form the basis of the topic.
Key Concepts
Gibbs Phenomenon: Refers to the overshoot and ringing seen when approximating discontinuous signals with Fourier series.
Ringing: The oscillations occurring in the vicinity of discontinuities in a signal's Fourier series representation.
Convergence Behavior: The analysis of how the Fourier series approaches the average of values around a discontinuity.
Overshoot Magnitude: The constant overshoot of approximately 9% of the jump at discontinuities.
See how the concepts apply in real-world scenarios to understand their practical implications.
In approximating a square wave using a Fourier series, adding terms improves smoothness but introduces ringing at the jumps.
For a discontinuous signal jumping from -1 to +1, the Fourier series will show overshooting behavior at each discontinuity.
Use mnemonics, acronyms, or visual cues to help remember key information more easily.
When the wave goes jump and skips, expect a ring, with many dips.
Imagine a tightrope walker suddenly leaping from one building to another; the perfect jump is tough to achieve just right, representing how hard it is for Fourier series to capture such jumps perfectly.
Gibbs Is Generally Boosted 9% (GIBBS) helps remember the overshoot percentage.
Review key concepts with flashcards.
Review the Definitions for terms.
Term: Gibbs Phenomenon
Definition:
An overshoot that occurs when a finite number of terms from a Fourier series approximates a signal with discontinuities, characterized by oscillations near the discontinuity.
Term: Ringing
Definition:
Oscillations that appear around the discontinuities of a Fourier series approximation.
Term: Convergence
Definition:
The behavior of a series approaching a specific value or average, especially at points of discontinuity.
Term: Windowing
Definition:
A technique used to reduce the Gibbs phenomenon by tapering the Fourier series coefficients.