The final Signals and Systems lecture explains how audio playback evolved from the fragile Edison cylinder phonograph to durable modern optical disks, through the application of digital signal processing concepts.

Lecture 25: Audio CD

Continuing the previous discussion of AM in radio, Prof. Freeman analyzes phase and frequency modulated (PM/FM) signals, before presenting research showing improvement in optical microscopy via phase-modulated illumination.

Lecture 24: Modulation, Part 2

Efficient signal transmission and reception requires wavelengths matching the size of the antenna; for speech, this requires frequencies around the GHz range. Broadcast radio developed AM and FM to produce accurate reception of multiplexed signals.

Lecture 23: Modulation, Part 1

Digital audio, images, video, and communication signals use quantization to create discrete representations of continuous phenomena. Efficient transmission and reconstruction uses techniques such as dithering, progressive refinement, and the JPEG encoding.

Lecture 22: Sampling and Quantization

Sampling produces a discrete-time (digital) signal from a continuous-time (physical) phenomenon. Anti-aliasing and reconstruction filters remove unnecessary frequencies while retaining enough information to reconstruct the original signal.

Lecture 21: Sampling

Three examples of Fourier transforms in action are given: removing noise from an electrocardiogram signal, using laser diffraction to calculate the groove spacing on CDs and DVDs, and determining the structure of DNA via x-ray crystallography.

Lecture 20: Applications of Fourier Transforms

Today's lecture solidifies the connections between continuous- and discrete-time Fourier series and transforms, converting between the time and frequency domains with familiar tools such as convolution, periodic extension, and sampling.

Lecture 19: Relations Among Fourier Representations

Continuing the comparison of continuous- and discrete-time signals, today's lecture discusses the DT Fourier transform, computation of Fourier series via the Fast Fourier Transform (FFT), and examples from digital image processing.

Lecture 18: Discrete-Time (DT) Fourier Representations

As digital signal processing components have become cheaper, traditional design problems in audio and video systems have converted to discrete-time. This lecture compares system responses and Fourier representations in discrete- and continuous-time.

Lecture 17: Discrete-Time (DT) Frequency Representations

The concept of the Fourier series can be applied to aperiodic functions by treating it as a periodic function with period T = infinity. This new transform has some key similarities and differences with the Laplace transform, its properties, and domains.

Lecture 16: Fourier Transform

Took this class in college, memorized a bunch of equations and had no idea what any of it meant. This MIT course does an amazing job explaining the practicality behind the equations and the real world applications. Video is a little blurry, hence the 4 stars. Otherwise absolutely phenomenal.

Just what I needed

Signals and Systems

Additional examples today illustrate the use of feedback to reduce sensitivity to variable component parameters and crossover distortion in audio systems, and to control two unstable systems (magnetic levitation, inverted pendulum).

Lecture 13: Continuous-Time (CT) Feedback and Control, Part 2

Bode plots are a simpler method of graphing the frequency response, using the poles and zeros of the system to construct asymptotes for each segment on a log-log plot. The Q factor affects the sharpness of peaks and drop-offs in the system.

Lecture 11: Continuous-Time (CT) Frequency Response and Bode Plot

The response of a system to sinusoidal input gives valuable information about its behavior in the frequency domain, similar to convolution in the time domain. Eigenfunctions and vector plots are used to explore this frequency response.

Lecture 9: Frequency Response

Building on concepts from the previous lecture, the Laplace transform is introduced as the continuous-time analogue of the Z transform. The lecture discusses the Laplace transform's definition, properties, applications, and inverse transform.

Lecture 6: Laplace Transform

After reviewing concepts in discrete-time systems, the Z transform is introduced, connecting the unit sample response h[n] and the system function H(z). The lecture covers the Z transform's definition, properties, examples, and inverse transform.

Lecture 5: Z Transform

Drawing analogies with previous concepts in discrete-time systems, this lecture discusses the block diagrams, polynomial expressions, poles, convergence regions, and fundamental modes of continuous-time systems.

Lecture 4: Continuous-Time (CT) Systems

To analyze complicated systems of adders, delays, and gains, factor their polynomial expression into simpler components using the poles. These fundamental modes combine to produce the unit response of a system.

Lecture 3: Feedback, Poles, and Fundamental Modes

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