Difference between revisions of "ECE 280/Spring 2024/Test 2"
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==Test II Coverage== | ==Test II Coverage== | ||
− | # Everything on [[ECE_280/ | + | # Everything on [[ECE_280/Spring 2024/Test_1|Test 1]] |
# Correlation - note that in previous semesters different versions of the correlation function may be used - the two possibilities are:<center><math>\begin{align*}\phi_{xy}&=\int_{-\infty}^{\infty}x(t+\tau)\,y(t)\,d\tau=x(t)*y(-t)=x(t)*y_{m}(t)=r_{xy}(-t)=r_{yx}(t)\\r_{xy}&=\int_{-\infty}^{\infty}x(\tau)\,y(t+\tau)\,d\tau=x(-t)*y(t)=x_m(t)*y(t)=\phi_{xy}(-t)=\phi_{yx}(t)\end{align*}</math></center>meaning the interpretation of the independent variable is different. For $$\phi_{xy}(t)$$, the "t" is "How far to the ''right'' do I slide $$y$$ for the area of the product of the signals to be $$\phi_{xy}(t)$$?"; alternately, it could be interpreted as "How far to the ''left'' do I slide $$x$$ for the area of the product of the signals to be equal to $$\phi_{xy}(t)$$?" For Fall 2023 for Dr. G's section, $$\phi_{xy}$$ will be used exclusively. | # Correlation - note that in previous semesters different versions of the correlation function may be used - the two possibilities are:<center><math>\begin{align*}\phi_{xy}&=\int_{-\infty}^{\infty}x(t+\tau)\,y(t)\,d\tau=x(t)*y(-t)=x(t)*y_{m}(t)=r_{xy}(-t)=r_{yx}(t)\\r_{xy}&=\int_{-\infty}^{\infty}x(\tau)\,y(t+\tau)\,d\tau=x(-t)*y(t)=x_m(t)*y(t)=\phi_{xy}(-t)=\phi_{yx}(t)\end{align*}</math></center>meaning the interpretation of the independent variable is different. For $$\phi_{xy}(t)$$, the "t" is "How far to the ''right'' do I slide $$y$$ for the area of the product of the signals to be $$\phi_{xy}(t)$$?"; alternately, it could be interpreted as "How far to the ''left'' do I slide $$x$$ for the area of the product of the signals to be equal to $$\phi_{xy}(t)$$?" For Fall 2023 for Dr. G's section, $$\phi_{xy}$$ will be used exclusively. | ||
# Linear constant-coefficient discrete difference equations | # Linear constant-coefficient discrete difference equations |
Revision as of 02:47, 27 March 2024
This page lists the topics covered on the second test for ECE 280 Spring 2024. This will cover everything through Homework 8 and all lecture material ending just before the start of Bode Plots. There are sample tests for Dr. G at Test Bank.
Test II Coverage
- Everything on Test 1
- Correlation - note that in previous semesters different versions of the correlation function may be used - the two possibilities are:
\(\begin{align*}\phi_{xy}&=\int_{-\infty}^{\infty}x(t+\tau)\,y(t)\,d\tau=x(t)*y(-t)=x(t)*y_{m}(t)=r_{xy}(-t)=r_{yx}(t)\\r_{xy}&=\int_{-\infty}^{\infty}x(\tau)\,y(t+\tau)\,d\tau=x(-t)*y(t)=x_m(t)*y(t)=\phi_{xy}(-t)=\phi_{yx}(t)\end{align*}\) meaning the interpretation of the independent variable is different. For $$\phi_{xy}(t)$$, the "t" is "How far to the right do I slide $$y$$ for the area of the product of the signals to be $$\phi_{xy}(t)$$?"; alternately, it could be interpreted as "How far to the left do I slide $$x$$ for the area of the product of the signals to be equal to $$\phi_{xy}(t)$$?" For Fall 2023 for Dr. G's section, $$\phi_{xy}$$ will be used exclusively. - Linear constant-coefficient discrete difference equations
- Fourier Series (Continuous Time only)
- Know the synthesis and analysis equations
- Be able to set up integrals or summations to determine \(x(t)\) or \(X[k]\) for periodic signals
- Know how to find the actual Fourier Series coefficients for periodic signals made up of cos and sin
- Be able to use the Fourier Series and Fourier Series Property tables
- Fourier Transform (Continuous Time)
- Know the synthesis and analysis equations
- Be able to set up integrals or summations to determine \(x(t)\) or \(X(j\omega)\) for signals that have Fourier Transforms
- Be able to use the Fourier Transform and Fourier Transform Property tables, including figuring out necessary adjustments to make things work for the tables
- Be able to use partial fraction expansion for inverse Fourier Transforms
Equation Sheet
See Canvas
Specifically Not On The Test
- Maple
- MATLAB
- Sampling and reconstruction
- Communication systems
- Laplace Transforms