Signals & Systems — Oppenheim, Willsky (2nd Edition)
Chapters 1–10: Key Theory & Practice Problems
Chapter 1: Signals and Systems
Key Concepts
- Continuous-Time (CT) Signals: Defined for every value of time $t$, denoted $x(t)$.
- Discrete-Time (DT) Signals: Defined only at integer values of $n$, denoted $x[n]$.
- Signal Energy and Power:
$$E_\infty = \int_{-\infty}^{\infty} |x(t)|^2\,dt \quad\text{(CT)}, \qquad E_\infty = \sum_{n=-\infty}^{\infty} |x[n]|^2 \quad\text{(DT)}$$$$P_\infty = \lim_{T\to\infty} \frac{1}{2T}\int_{-T}^{T} |x(t)|^2\,dt \quad\text{(CT average power)}$$
- Transformations of Independent Variable:
- Time shift: $x(t - t_0)$ shifts right by $t_0$
- Time reversal: $x(-t)$ reflects about $t = 0$
- Time scaling: $x(at)$, compressed if $|a| > 1$, expanded if $|a| < 1$
- Periodic Signals: $x(t) = x(t + T)$ for all $t$. Fundamental period $T_0$ is the smallest positive $T$.
- Even and Odd Decomposition:
$$\text{Ev}\{x(t)\} = \tfrac{1}{2}[x(t) + x(-t)], \qquad \text{Od}\{x(t)\} = \tfrac{1}{2}[x(t) - x(-t)]$$
- Complex Exponential Signals:
$$\text{CT: } x(t) = Ce^{st}, \quad s = \sigma + j\omega \qquad\qquad \text{DT: } x[n] = Cz^n, \quad z = re^{j\omega}$$CT complex exponentials with distinct frequencies are always distinct. DT complex exponentials are periodic in frequency with period $2\pi$.
- Unit Impulse and Unit Step:
$$\text{DT: } \delta[n] = \begin{cases}1, & n=0\\0, & n\ne 0\end{cases}, \quad u[n] = \begin{cases}1, & n\ge 0\\0, & n < 0\end{cases}, \quad \delta[n] = u[n] - u[n-1]$$$$\text{CT: } u(t) = \begin{cases}1, & t>0\\0, & t<0\end{cases}, \quad \delta(t) = \frac{du(t)}{dt}, \quad \int_{-\infty}^{\infty}\delta(t)\,dt = 1$$
- System Properties:
- Memoryless: Output depends only on current input
- Invertible: Distinct inputs produce distinct outputs
- Causal: Output depends only on present and past inputs
- Stable (BIBO): Bounded input $\Rightarrow$ bounded output
- Time-Invariant: Time shift in input $\Rightarrow$ same time shift in output
- Linear: Superposition: $T\{ax_1 + bx_2\} = aT\{x_1\} + bT\{x_2\}$
Problems and Solutions
Compute the total energy of $x(t) = e^{-2t}u(t)$.
Solution
Explanation
General definition. Signal energy is the integral (or sum) of the squared magnitude:
The $|\cdot|^2$ handles complex signals; for real signals it reduces to $x^2$. Classification:
- Energy signal: $0 < E < \infty$ (e.g., a pulse or decaying exponential).
- Power signal: $E = \infty$ but average power $P = \lim_{T\to\infty}\frac{1}{2T}\int_{-T}^{T}|x(t)|^2 dt$ is finite.
- A signal is one or the other (or neither), never both.
By Parseval's theorem, energy is preserved between time and frequency domains: $\int |x(t)|^2 dt = \frac{1}{2\pi}\int |X(\omega)|^2 d\omega$.
Apply to $x(t) = e^{-2t}u(t)$. The unit step $u(t)$ restricts the integral to $t \ge 0$, where $x(t) = e^{-2t}$:
$E = \tfrac{1}{4}$ J — finite, so $x(t)$ is an energy signal.
Given $x(t)$ defined for $0 \le t \le 2$, sketch $x(2t - 3)$.
Solution
Step 1: Replace $t$ with $t-3$: shift right by 3 → $x(t-3)$, defined on $[3, 5]$.
Step 2: Replace $t$ with $2t$: compress by factor 2 → $x(2t-3)$, defined when $0 \le 2t-3 \le 2$, i.e., $\frac{3}{2} \le t \le \frac{5}{2}$.
The signal is compressed by 2 and shifted to $[1.5,\; 2.5]$.
Decompose $x(t) = e^{t}u(t)$ into even and odd parts.
Solution
Determine if $x[n] = \cos\!\left(\frac{6\pi n}{7}\right)$ is periodic. If so, find the fundamental period.
Solution
$\omega_0 = \frac{6\pi}{7}$. For periodicity, we need $\omega_0 N = 2\pi m$:
Smallest integer $N$: $m=3 \Rightarrow N=7$. The signal is periodic with fundamental period $N=7$.
Is $x(t) = \cos(2t) + \sin(\pi t)$ periodic?
Solution
$T_1 = \frac{2\pi}{2} = \pi$, $\;T_2 = \frac{2\pi}{\pi} = 2$. Ratio $\frac{T_1}{T_2} = \frac{\pi}{2}$ is irrational.
Since the ratio of periods is irrational, the sum is not periodic.
Determine if the system $y(t) = t\cdot x(t)$ is linear.
Solution
Let $x_3(t) = ax_1(t)+bx_2(t)$. Then:
Superposition holds $\Rightarrow$ the system is linear.
Is the system $y[n] = n\cdot x[n]$ time-invariant?
Solution
Shift input: $x_1[n] = x[n-n_0] \Rightarrow y_1[n] = n\,x[n-n_0]$.
Shift output: $y[n-n_0] = (n-n_0)\,x[n-n_0]$.
Since $n\,x[n-n_0] \ne (n-n_0)\,x[n-n_0]$, the system is not time-invariant.
Determine if $y(t) = x(t-2)$ is (a) causal, (b) stable.
Solution
(a) Output at time $t$ depends on $x(t-2)$ (past input). The system is causal.
(b) If $|x(t)| \le M$, then $|y(t)| = |x(t-2)| \le M$. The system is BIBO stable.
Compute the average power of $x(t) = A\cos(\omega_0 t + \phi)$.
Solution
The average power of a sinusoid is half the square of its amplitude.
For $y(t) = \int_{-\infty}^{t} x(\tau)\,d\tau$, determine linearity, time-invariance, causality, and stability.
Solution
Linear: Yes — integration is linear.
Time-Invariant: Yes — shifting input by $t_0$ shifts output by $t_0$.
Causal: Yes — integrates from $-\infty$ to present time $t$.
Stable: No — $x(t)=u(t)$ (bounded) gives $y(t)=t\,u(t)$ (unbounded).
Chapter 2: Linear Time-Invariant Systems
Key Concepts
- Convolution Sum (DT): Any DT signal: $x[n] = \sum_k x[k]\,\delta[n-k]$. For LTI systems:
$$y[n] = x[n] * h[n] = \sum_{k=-\infty}^{\infty} x[k]\,h[n-k]$$
- Convolution Integral (CT):
$$y(t) = x(t) * h(t) = \int_{-\infty}^{\infty} x(\tau)\,h(t-\tau)\,d\tau$$
- Properties of Convolution:
- Commutative: $x*h = h*x$
- Distributive: $x*(h_1+h_2) = x*h_1 + x*h_2$
- Associative: $x*(h_1*h_2) = (x*h_1)*h_2$
- Identity: $x[n]*\delta[n] = x[n]$
- LTI System Properties via $h(t)$ or $h[n]$:
- Memoryless: $h[n] = K\delta[n]$
- Causal: $h(t) = 0$ for $t < 0$
- Stable: $\int_{-\infty}^{\infty}|h(t)|\,dt < \infty$ or $\sum_{n}|h[n]| < \infty$
- Linear Constant-Coefficient Differential/Difference Equations:
$$\text{CT: } \sum_{k=0}^{N} a_k \frac{d^k y}{dt^k} = \sum_{k=0}^{M} b_k \frac{d^k x}{dt^k}$$$$\text{DT: } \sum_{k=0}^{N} a_k\, y[n-k] = \sum_{k=0}^{M} b_k\, x[n-k]$$
- Unit Step Response: $s(t) = \int_{-\infty}^{t} h(\tau)\,d\tau$, so $h(t) = \dfrac{ds(t)}{dt}$
Problems and Solutions
Compute $y[n] = x[n]*h[n]$ where $x[n] = \{1, 2, 1\}$ and $h[n] = \{1, 1, 1\}$ (both starting at $n=0$).
Solution
$y[n] = \{1, 3, 4, 3, 1\}$ for $n = 0,1,2,3,4$.
Compute $y(t) = e^{-t}u(t) * u(t)$.
Solution
Compute $y(t) = e^{-at}u(t) * e^{-bt}u(t)$ for $a \ne b$.
Solution
Determine if the system with $h(t) = e^{2t}u(-t)$ is stable.
Solution
The integral converges $\Rightarrow$ stable.
Is the system with $h[n] = \left(\frac{1}{3}\right)^n u[n] + \left(\frac{1}{2}\right)^n u[n]$ causal and stable?
Solution
Causal: $h[n] = 0$ for $n < 0$ (both terms have $u[n]$) $\Rightarrow$ yes.
Stable:
Two LTI systems in cascade: $h_1(t) = e^{-t}u(t)$ and $h_2(t) = e^{-2t}u(t)$. Find the overall impulse response.
Solution
Find the impulse response of $y[n] - \tfrac{1}{2}y[n-1] = x[n]$, assuming causality.
Solution
For $x[n] = \delta[n]$ with initial rest:
Given $h(t) = e^{-3t}u(t)$, find the unit step response $s(t)$.
Solution
Find $h(t)$ for $\dfrac{dy}{dt} + 2y(t) = x(t)$, assuming causality.
Solution
Compute $y[n] = x[n] * \bigl(\delta[n] + \delta[n-2]\bigr)$ where $x[n] = a^n u[n]$.
Solution
Chapter 3: Fourier Series Representation of Periodic Signals
Key Concepts
- Eigenfunctions of LTI Systems: If $x(t) = e^{st}$, then $y(t) = H(s)\,e^{st}$. Complex exponentials are eigenfunctions of LTI systems.
- CT Fourier Series: For a periodic signal with period $T$, $\omega_0 = 2\pi/T$:
$$x(t) = \sum_{k=-\infty}^{\infty} a_k\, e^{jk\omega_0 t}$$$$a_k = \frac{1}{T}\int_{T} x(t)\, e^{-jk\omega_0 t}\,dt$$
- DT Fourier Series: For period $N$, $\omega_0 = 2\pi/N$:
$$x[n] = \sum_{k=\langle N\rangle} a_k\, e^{jk(2\pi/N)n}, \qquad a_k = \frac{1}{N}\sum_{n=\langle N\rangle} x[n]\, e^{-jk(2\pi/N)n}$$
- Convergence (Dirichlet Conditions): Absolutely integrable over one period; finite maxima/minima; finite discontinuities.
- Parseval's Relation:
$$\frac{1}{T}\int_T |x(t)|^2\,dt = \sum_{k=-\infty}^{\infty}|a_k|^2 \qquad\text{(CT)}$$$$\frac{1}{N}\sum_{n=\langle N\rangle}|x[n]|^2 = \sum_{k=\langle N\rangle}|a_k|^2 \qquad\text{(DT)}$$
- Key Properties: Linearity; time shift $\to$ phase change $a_k e^{-jk\omega_0 t_0}$; conjugate symmetry for real signals $a_k = a_{-k}^*$; multiplication $\to$ convolution of coefficients.
- Frequency Response: For periodic input, output coefficients: $b_k = H(jk\omega_0)\,a_k$.
Problems and Solutions
Find the Fourier series coefficients of a square wave: $x(t)=1$ for $|t|Solution
Find the Fourier series coefficients of $x(t) = \cos(3t)$.
Solution
Find the Fourier series of $x[n] = \cos(2\pi n/4)$ with period $N=4$.
Solution
$a_1 = \frac{1}{2}$, $a_3 = a_{-1} = \frac{1}{2}$ (since period 4), $a_0 = a_2 = 0$.
Given the square wave from 3.1 with $T_1 = T/4$, compute $\sum|a_k|^2$.
Solution
If $x(t)$ has coefficients $a_k$, find the coefficients of $y(t) = x(t - t_0)$.
Solution
Magnitudes $|b_k| = |a_k|$ are unchanged; only phase shifts.
For $H(j\omega) = \frac{1}{1+j\omega RC}$, find the output Fourier coefficients for a square wave input with $a_k = \frac{\sin(k\pi/2)}{k\pi}$.
Solution
Higher harmonics are attenuated by the lowpass filter.
Find the Fourier series of $x[n] = \sum_r \delta[n-rN]$ (periodic impulse train, period $N$).
Solution
All harmonics have equal amplitude $1/N$.
Find the Fourier series of $x(t) = t/T$ for $-T/2 < t < T/2$.
Solution
Find the DT Fourier series for $x[n]$ periodic with $N=5$: $x[n]=1$ for $n=0,1,2$ and $x[n]=0$ for $n=3,4$.
Solution
A system has $H(j\omega) = j\omega$. If input has coefficients $a_k$, find output coefficients.
Solution
This differentiator amplifies higher harmonics linearly with frequency.
Chapter 4: The Continuous-Time Fourier Transform
Key Concepts
- Fourier Transform Pair:
$$X(j\omega) = \int_{-\infty}^{\infty} x(t)\, e^{-j\omega t}\,dt \qquad\text{(Analysis)}$$$$x(t) = \frac{1}{2\pi}\int_{-\infty}^{\infty} X(j\omega)\, e^{j\omega t}\,d\omega \qquad\text{(Synthesis)}$$
- FT of Periodic Signals:
$$x(t) = \sum_k a_k e^{jk\omega_0 t} \;\Longrightarrow\; X(j\omega) = 2\pi\sum_k a_k\,\delta(\omega - k\omega_0)$$
- Key Transform Pairs:
$$e^{-at}u(t) \longleftrightarrow \frac{1}{a+j\omega},\; a>0 \qquad \delta(t) \longleftrightarrow 1 \qquad 1 \longleftrightarrow 2\pi\delta(\omega)$$
- Properties:
- Time shift: $x(t-t_0) \longleftrightarrow e^{-j\omega t_0}X(j\omega)$
- Frequency shift: $e^{j\omega_0 t}x(t) \longleftrightarrow X(j(\omega-\omega_0))$
- Differentiation: $\frac{dx}{dt} \longleftrightarrow j\omega\, X(j\omega)$
- Convolution: $x*h \longleftrightarrow X\cdot H$
- Multiplication: $x\cdot h \longleftrightarrow \frac{1}{2\pi}X*H$
- Scaling: $x(at) \longleftrightarrow \frac{1}{|a|}X\!\left(\frac{j\omega}{a}\right)$
- Parseval: $\int|x(t)|^2 dt = \frac{1}{2\pi}\int|X(j\omega)|^2 d\omega$
- Duality: $X(jt) \longleftrightarrow 2\pi\, x(-\omega)$
Problems and Solutions
Find $X(j\omega)$ for $x(t) = e^{-3t}u(t)$.
Solution
Find $X(j\omega)$ for $x(t) = e^{-|t|}$.
Solution
Find $x(t)$ given $X(j\omega) = 2\pi\delta(\omega) + \pi\delta(\omega-4) + \pi\delta(\omega+4)$.
Solution
Find $y(t) = e^{-2t}u(t) * e^{-3t}u(t)$ using Fourier transforms.
Solution
Find the FT of $y(t) = \frac{dx}{dt}$ where $x(t) = e^{-t}u(t)$.
Solution
Note: $y(t) = \delta(t) - e^{-t}u(t)$, consistent with $\mathcal{F}\{\delta\}=1$.
Compute $\int_{-\infty}^{\infty}|X(j\omega)|^2\,d\omega$ where $X(j\omega) = \frac{1}{1+j\omega}$.
Solution
Find the FT of $x(t) = 1$ for $|t| \le T$, $0$ otherwise.
Solution
Find the FT of $y(t) = x(t)\cos(\omega_c t)$ in terms of $X(j\omega)$.
Solution
Multiplying by $\cos$ shifts the spectrum to $\pm\omega_c$ (amplitude modulation).
$H(j\omega) = \frac{1}{2+j\omega}$, input $x(t) = e^{-t}u(t)$. Find $y(t)$.
Solution
Find the FT of $x(t) = \sum_{n=-\infty}^{\infty}\delta(t - nT)$.
Solution
The FT of an impulse train with period $T$ is an impulse train with period $\omega_s = 2\pi/T$.
Chapter 5: The Discrete-Time Fourier Transform
Key Concepts
- DTFT Pair:
$$X(e^{j\omega}) = \sum_{n=-\infty}^{\infty} x[n]\, e^{-j\omega n} \qquad\text{(Analysis)}$$$$x[n] = \frac{1}{2\pi}\int_{2\pi} X(e^{j\omega})\, e^{j\omega n}\,d\omega \qquad\text{(Synthesis)}$$
- Key property: $X(e^{j\omega})$ is always periodic in $\omega$ with period $2\pi$.
- Common Pairs:
$$a^n u[n] \;\longleftrightarrow\; \frac{1}{1-ae^{-j\omega}}, \quad |a|<1 \qquad\qquad \delta[n] \;\longleftrightarrow\; 1$$
- Properties:
- Time shift: $x[n-n_0] \longleftrightarrow e^{-j\omega n_0}X(e^{j\omega})$
- Frequency shift: $e^{j\omega_0 n}x[n] \longleftrightarrow X(e^{j(\omega-\omega_0)})$
- Convolution: $x*h \longleftrightarrow X\cdot H$
- Differencing: $x[n]-x[n-1] \longleftrightarrow (1-e^{-j\omega})X(e^{j\omega})$
- Time expansion: $x_{(k)}[n] \longleftrightarrow X(e^{jk\omega})$
- Parseval: $\sum|x[n]|^2 = \frac{1}{2\pi}\int_{2\pi}|X(e^{j\omega})|^2\,d\omega$
Problems and Solutions
Find $X(e^{j\omega})$ for $x[n] = (0.5)^n u[n]$.
Solution
Find $X(e^{j\omega})$ for $x[n] = 1$ for $0 \le n \le 4$, else $0$.
Solution
Find $x[n]$ if $X(e^{j\omega}) = 1$ for $|\omega| \le W$, $0$ for $W < |\omega| \le \pi$.
Solution
This is the inverse DTFT of an ideal lowpass filter.
Find $y[n] = (0.5)^n u[n] * (0.25)^n u[n]$.
Solution
If $X(e^{j\omega}) = \frac{1}{1-0.5e^{-j\omega}}$, find the DTFT of $x[n-3]$.
Solution
Find $\sum_{n=-\infty}^{\infty}|(0.8)^n u[n]|^2$.
Solution
Find the DTFT of $x[n] = a^{|n|}$ for $|a|<1$.
Solution
Find $H(e^{j\omega})$ for $y[n] - 0.5y[n-1] = x[n] + x[n-1]$.
Solution
$|H(e^{j0})| = 2/0.5 = 4$, $|H(e^{j\pi})| = 0/1.5 = 0$ $\Rightarrow$ lowpass filter.
Find the DTFT of $u[n]$.
Solution
Includes an impulse at $\omega=0$ since $u[n]$ is not absolutely summable.
$y[n] = \sum_{k=-\infty}^{n} x[k]$. Find $H(e^{j\omega})$.
Solution
The DT analogue of integration.
Chapter 6: Time and Frequency Characterization of Signals and Systems
Key Concepts
- Magnitude-Phase: $H(j\omega) = |H(j\omega)|\,e^{j\angle H(j\omega)}$. Output: $|Y|=|H||X|$, $\angle Y = \angle H + \angle X$.
- Linear Phase: $H(j\omega) = |H(j\omega)|\,e^{-j\omega t_d}$ means pure delay $t_d$ with no distortion.
- Group Delay:
$$\tau(\omega) = -\frac{d\,\angle H(j\omega)}{d\omega}$$
- Bode Plots: $20\log_{10}|H(j\omega)|$ in dB vs $\log\omega$.
- First-order pole at $-a$: $-20$ dB/decade above $\omega=a$
- First-order zero at $-a$: $+20$ dB/decade above $\omega=a$
- Ideal Filters: Impulse response is sinc (non-causal). Sharp cutoff $\Leftrightarrow$ infinite time response.
- Second-Order System:
$$H(j\omega) = \frac{\omega_n^2}{\omega_n^2 - \omega^2 + 2j\zeta\omega_n\omega}$$
Problems and Solutions
Sketch the Bode magnitude plot for $H(j\omega) = \dfrac{10(j\omega+1)}{(j\omega+10)(j\omega+100)}$.
Solution
DC gain: $H(0) = \frac{10}{1000} = 0.01 = -40$ dB.
Zero at $\omega=1$: $+20$ dB/dec. Pole at $\omega=10$: net flat. Pole at $\omega=100$: $-20$ dB/dec.
Flat at $-40$dB until $\omega=1$, rises to $-20$dB at $\omega=10$, flat to $\omega=100$, then $-20$dB/dec.
Find $h(t)$ for an ideal lowpass filter with cutoff $\omega_c$ and unit gain.
Solution
Non-causal ($h(t)\ne 0$ for $t<0$), so ideal filters are not realizable.
RC filter: $R=1\,\text{k}\Omega$, $C=1\,\mu\text{F}$. Find the 3dB cutoff.
Solution
$\omega_n = 10$, $\zeta = 0.1$. Find resonant frequency and peak gain.
Solution
Show that $\angle H(j\omega) = -\alpha\omega$ with $|H|=K$ introduces no distortion.
Solution
Scaled, delayed copy of input — no distortion.
Classify $H(e^{j\omega}) = \frac{1}{1-0.9e^{-j\omega}}$.
Solution
Lowpass filter with gain concentrated near $\omega=0$.
Show $|H(j\omega)| = 1$ for $H(j\omega) = \frac{j\omega - a}{j\omega + a}$, $a>0$.
Solution
$y[n] = \frac{1}{M}\sum_{k=0}^{M-1} x[n-k]$ with $M=4$. Find $H(e^{j\omega})$.
Solution
Lowpass filter with nulls at $\omega = \pi/2,\;\pi,\; 3\pi/2$.
Explain the tradeoff between transition bandwidth and time-domain ringing.
Solution
Sharper transition band $\Rightarrow$ longer impulse response $\Rightarrow$ more ringing. Shorter impulse response $\Rightarrow$ wider transition band. This is the time-frequency uncertainty principle.
First-order system $H(j\omega) = \frac{1}{1+j\omega/\omega_c}$. Relate rise time to bandwidth.
Solution
Chapter 7: Sampling
Key Concepts
- Sampling Theorem (Nyquist): A bandlimited signal with $X(j\omega)=0$ for $|\omega|>\omega_M$ is uniquely determined by its samples if:
$$\omega_s = \frac{2\pi}{T} \ge 2\omega_M \qquad\text{(Nyquist rate)}$$
- Impulse-Train Sampling:
$$X_s(j\omega) = \frac{1}{T}\sum_{k=-\infty}^{\infty} X(j(\omega - k\omega_s))$$Spectrum replicates at multiples of $\omega_s$.
- Reconstruction: Ideal lowpass with cutoff $\omega_s/2$, gain $T$:
$$x(t) = \sum_{n=-\infty}^{\infty} x(nT)\,\frac{\sin\bigl(\omega_c(t-nT)\bigr)}{\omega_c(t-nT)/\pi}$$
- Aliasing: If $\omega_s < 2\omega_M$, spectral copies overlap — irreversible distortion.
- Zero-Order Hold:
$$H_0(j\omega) = T\,e^{-j\omega T/2}\,\frac{\sin(\omega T/2)}{\omega T/2}$$
- DT Processing of CT Signals: $H_{\text{eff}}(j\omega) = H(e^{j\omega T})$ for $|\omega|<\pi/T$.
- Decimation/Interpolation: Downsampling by $M$, upsampling by $L$.
Problems and Solutions
Find the Nyquist rate for $x(t) = 3\cos(50\pi t) + 10\sin(300\pi t) - \cos(100\pi t)$.
Solution
$x(t) = \cos(2\pi\cdot 100\,t)$ sampled at $f_s = 250$ Hz. Reconstructed frequency?
Solution
$f = 100 < f_s/2 = 125$ Hz $\Rightarrow$ no aliasing. Reconstructed signal: $\cos(2\pi\cdot 100\,t)$.
$x(t) = \cos(2\pi\cdot 300\,t)$ sampled at $f_s = 500$ Hz. What frequency appears?
Solution
$X(j\omega) = 0$ for $|\omega| > 1000\pi$. Maximum $T$?
Solution
Samples: $x[0]=1,\;x[1]=0,\;x[2]=-1,\;x[3]=0$ with $T=1$, ideal lowpass at $\omega_c=\pi$.
Solution
Describe the frequency response of a ZOH and its effect.
Solution
Sinc-shaped magnitude causes droop at higher frequencies; introduces delay $T/2$.
CT signal ($\omega_M=2000\pi$) sampled at $\omega_s=8000\pi$. What CT frequency does $|\omega|\le\pi/4$ correspond to?
Solution
Signal up to 5 kHz, sampling at 8 kHz. Design anti-aliasing filter.
Solution
Nyquist: $f_s/2 = 4$ kHz $<$ 5 kHz $\Rightarrow$ aliasing. Need lowpass with cutoff $\le 4$ kHz to remove 4–5 kHz content before sampling.
$X(e^{j\omega}) = 0$ for $\pi/3 < |\omega| \le \pi$. Downsample by 3: $y[n] = x[3n]$.
Solution
Since $X$ is bandlimited to $|\omega|<\pi/3$, no overlap: $Y(e^{j\omega}) = \frac{1}{3}X(e^{j\omega/3})$.
Describe DT interpolation by factor 2.
Solution
Insert one zero between samples, then lowpass filter with cutoff $\pi/2$ and gain 2:
Chapter 8: Communication Systems
Key Concepts
- Amplitude Modulation:
$$y(t) = x(t)\cos(\omega_c t) \;\Longrightarrow\; Y(j\omega) = \tfrac{1}{2}X(j(\omega-\omega_c)) + \tfrac{1}{2}X(j(\omega+\omega_c))$$
- Synchronous Demodulation:
$$y(t)\cos(\omega_c t) = \tfrac{1}{2}x(t) + \tfrac{1}{2}x(t)\cos(2\omega_c t) \;\xrightarrow{\;\text{LPF}\;}\; \tfrac{1}{2}x(t)$$
- Asynchronous (Envelope) Detection: $y(t) = [A+x(t)]\cos(\omega_c t)$. Works when $A+x(t)>0$.
- FDM: Signals modulated to different carriers share one channel.
- SSB: Transmit one sideband only — saves half the bandwidth.
- FM: $\omega_i(t) = \omega_c + k_f x(t)$. More bandwidth but better noise immunity than AM.
- Carson's Rule: $\text{BW} \approx 2(\Delta f + f_m)$.
- TDM: Signals interleaved in time.
Problems and Solutions
$x(t)$ has bandwidth $W=5$ kHz. Bandwidth of $y(t) = x(t)\cos(2\pi\cdot 100\text{k}\cdot t)$?
Solution
Spectrum at $[95, 105]$ kHz $\cup$ $[-105, -95]$ kHz.
$y(t) = x(t)\cos(100t)$ demodulated by $\cos(100t)$ then lowpass. Output if BW of $x$ is 10 rad/s?
Solution
Demodulating carrier has phase error $\phi$. Output?
Solution
Attenuation by $\cos\phi$. At $\phi=90°$, output is zero.
Three 4 kHz signals, 1 kHz guard bands.
Solution
Compare bandwidth for 5 kHz baseband.
Solution
$y(t) = [A+x(t)]\cos(\omega_c t)$, $\max|x(t)|=1$. Minimum $A$?
Solution
Conventional AM with tone modulation at index $m$.
Solution
At $m=1$: $\eta = \frac{1}{3} = 33\%$. Most power is in the carrier.
Show that for $\beta \ll 1$, FM bandwidth $\approx$ AM bandwidth.
Solution
Bandwidth $= 2f_m$, same as AM.
$f_m = 15$ kHz, $\Delta f = 75$ kHz.
Solution
4 signals, each 4 kHz bandwidth, TDM multiplexed.
Solution
Chapter 9: The Laplace Transform
Key Concepts
- Bilateral Laplace Transform:
$$X(s) = \int_{-\infty}^{\infty} x(t)\,e^{-st}\,dt, \qquad s = \sigma + j\omega$$Fourier transform is the special case $X(j\omega) = X(s)\big|_{s=j\omega}$ when $j\omega$ axis is in ROC.
- Region of Convergence (ROC):
- Right-sided signal: ROC right of the rightmost pole
- Left-sided signal: ROC left of the leftmost pole
- Two-sided signal: strip between poles
- Causal + stable $\Rightarrow$ all poles in LHP, ROC includes $j\omega$ axis
- Common Pairs:
$$e^{-at}u(t) \;\longleftrightarrow\; \frac{1}{s+a},\;\text{ROC: Re}\{s\}>-a$$$$-e^{-at}u(-t) \;\longleftrightarrow\; \frac{1}{s+a},\;\text{ROC: Re}\{s\}<-a$$
- Properties: Time shift ($e^{-st_0}X(s)$), $s$-domain shift, differentiation ($sX(s)$), convolution ($X\cdot H$), initial/final value theorems.
- Unilateral Transform: Integration from $0^-$ to $\infty$. For ODEs with initial conditions.
Problems and Solutions
Find $X(s)$ and ROC for $x(t) = e^{-2t}u(t) + e^{-3t}u(t)$.
Solution
$X(s) = \frac{2s+4}{(s+1)(s+3)}$, ROC: Re$\{s\}>-1$.
Solution
$H(s) = \frac{s+1}{(s+2)(s+3)}$. Is the causal system stable?
Solution
Zero at $s=-1$. Poles at $s=-2, -3$ (both in LHP).
$\frac{dy}{dt}+3y = e^{-t}u(t)$, $y(0^-)=1$.
Solution
$y(t) = te^{-t}u(t) * e^{-2t}u(t)$.
Solution
$X(s) = \frac{3s+7}{(s+1)(s+2)}$.
Solution
$\frac{d^2y}{dt^2} + 5\frac{dy}{dt} + 6y = \frac{dx}{dt} + x$.
Solution
(a) $H(s) = \frac{1}{s^2+4}$, (b) $H(s) = \frac{1}{s^2+2s+5}$.
Solution
(a) Poles at $s = \pm 2j$ (imaginary axis) $\Rightarrow$ marginally stable.
(b) Poles at $s = -1\pm 2j$ (LHP) $\Rightarrow$ stable.
Forward path $G(s)=\frac{10}{s+1}$, feedback $H(s)=1$. Closed-loop TF?
Solution
Feedback moves the pole from $s=-1$ to $s=-11$.
$X(s) = \frac{1}{(s+1)(s-2)}$. Find all possible $x(t)$.
Solution
Partial fractions: $X(s) = \frac{1}{3}\!\left[\frac{-1}{s+1}+\frac{1}{s-2}\right]$.
Chapter 10: The z-Transform
Key Concepts
- z-Transform:
$$X(z) = \sum_{n=-\infty}^{\infty} x[n]\,z^{-n}, \qquad z = re^{j\omega}$$DTFT: $X(e^{j\omega}) = X(z)\big|_{z=e^{j\omega}}$ when unit circle is in ROC.
- ROC Rules:
- Causal (right-sided): ROC outside outermost pole
- Left-sided: ROC inside innermost pole
- Finite-length: entire $z$-plane (possibly excluding $z=0$ or $\infty$)
- Causal + stable: all poles inside unit circle
- Common Pairs:
$$a^n u[n] \;\longleftrightarrow\; \frac{1}{1-az^{-1}} = \frac{z}{z-a}, \quad\text{ROC: }|z|>|a|$$$$-a^n u[-n-1] \;\longleftrightarrow\; \frac{1}{1-az^{-1}}, \quad\text{ROC: }|z|<|a|$$
- Properties: Time shift ($z^{-n_0}X(z)$), convolution ($X\cdot H$), $z$-domain differentiation ($-z\frac{dX}{dz} \longleftrightarrow n\,x[n]$).
- System Analysis: $H(z)=Y(z)/X(z)$. Causal+stable $\Leftrightarrow$ all poles inside unit circle. FIR: always stable.
- Mapping: $z = e^{sT}$ relates $z$-transform to Laplace through sampling.
Problems and Solutions
$x[n] = (0.5)^n u[n]$.
Solution
$x[n] = (0.5)^n u[n] + (-\frac{1}{3})^n u[-n-1]$.
Solution
First term ROC: $|z|>0.5$. Second term (left-sided): ROC $|z|<\frac{1}{3}$.
Intersection is empty ($\frac{1}{3}<0.5$) $\Rightarrow$ z-transform does not exist for this signal.
$X(z) = \frac{z}{(z-0.5)(z-0.25)}$, ROC: $|z|>0.5$.
Solution
$y[n] - 0.5y[n-1] + 0.06y[n-2] = x[n]$.
Solution
Poles at $z=0.2, 0.3$ — both inside unit circle $\Rightarrow$ causal and stable.
$y[n] = x[n] - x[n-2]$.
Solution
Causal system: $H(z) = \frac{1}{1-1.5z^{-1}}$. Stable?
Solution
Not stable.
$y[n]-0.5y[n-1] = \delta[n]+\delta[n-1]$, $y[-1]=2$. Unilateral z-transform.
Solution
$H(z) = \frac{1+2z^{-1}}{1-0.5z^{-1}}$.
Solution
One delay element stores $w[n-1]$, used in both paths.
Zero at $z=1$, pole at $z=0.95$. Sketch $|H(e^{j\omega})|$.
Solution
Highpass filter.
Show how $z = e^{sT}$ connects $z$-transform to Laplace.
Solution
Key mapping:
Stable CT (poles in LHP) $\Leftrightarrow$ stable DT (poles inside unit circle).
Others — Residual Problems
Auxiliary problems moved out of the main 10-problem-per-chapter set. Useful but secondary in priority.
Chapter 1: Signals and Systems
Express the rectangular pulse $p(t) = 1$ for $|t| \le 1$, $0$ otherwise, using unit step functions.
Solution
Compute the energy of $x[n] = \left(\frac{1}{2}\right)^n u[n]$.
Solution
Classify: (a) $y[n] = x[n]^2$, (b) $y[n] = x[n-1]$.
Solution
(a) Output depends only on current input $\Rightarrow$ memoryless.
(b) Output depends on past input $\Rightarrow$ has memory.
Is the system $y(t) = x^2(t)$ invertible?
Solution
Both $x(t)$ and $-x(t)$ produce the same output $y(t) = x^2(t)$. Distinct inputs map to the same output $\Rightarrow$ not invertible.
Show that $e^{j\omega n} = e^{j(\omega+2\pi)n}$ for all integer $n$.
Solution
Since $n$ is an integer, $e^{j2\pi n}=1$. DT complex exponentials are periodic in frequency with period $2\pi$.
Chapter 2: Linear Time-Invariant Systems
Compute $x(t) * \delta(t-3)$.
Solution
Convolution with a shifted impulse simply shifts the signal.
Compute the convolution of $p(t) = u(t) - u(t-1)$ with itself.
Solution
The result is a triangular pulse.
$h_1[n] = \left(\frac{1}{2}\right)^n u[n]$ and $h_2[n] = -\left(\frac{1}{3}\right)^n u[n]$ in parallel.
Solution
Verify $x[n]*h[n] = h[n]*x[n]$ for $x[n] = \delta[n] + 2\delta[n-1]$ and $h[n] = u[n]-u[n-3]$.
Solution
$h[n] = \{1,1,1\}$ for $n=0,1,2$.
Both identical $\Rightarrow$ commutativity verified.
Show that the system with $h(t) = u(t)$ is not BIBO stable.
Solution
Counterexample: $x(t)=u(t)$ gives $y(t)=t\,u(t) \to \infty$. Not stable.
Chapter 3: Fourier Series
Show that for a real, even periodic signal, $a_k$ is real and even.
Solution
Real signal: $a_k = a_{-k}^*$ (conjugate symmetry).
Even signal: $a_k = a_{-k}$.
Combining: $a_k = a_k^* \Rightarrow a_k$ is real. And $a_k = a_{-k} \Rightarrow$ even.
If $x(t)$ has coefficients $a_k$ and $y(t)$ has $b_k$ (same period), find $c_k$ for $z(t)=x(t)y(t)$.
Solution
Multiplication in time $\longleftrightarrow$ convolution of coefficients.
Explain the Gibbs phenomenon for the Fourier series of a square wave.
Solution
Truncating to $N$ terms causes oscillatory overshoot near discontinuities. As $N\to\infty$, the overshoot narrows but never vanishes, with peak overshoot $\approx 9\%$ of the discontinuity height.
$y[n] = \frac{1}{2}y[n-1] + x[n]$ receives periodic input with period 4. Find output coefficients.
Solution
$a_0=1$, $a_1=a_{-1}=0.5$, $a_2=a_{-2}=0.2$, all others $0$. Find the average power.
Solution
DC power fraction: $1/1.58 = 63.3\%$. Fundamental: $0.5/1.58 = 31.6\%$.
Chapter 4: CT Fourier Transform
If $X(j\omega) = \frac{1}{1+j\omega}$, find the FT of $x(2t)$.
Solution
Use duality to find the FT of $x(t) = \frac{1}{1+t^2}$.
Solution
Known: $e^{-|t|} \longleftrightarrow \frac{2}{1+\omega^2}$. By duality: $\frac{2}{1+t^2} \longleftrightarrow 2\pi\,e^{-|\omega|}$.
Find the FT of $y(t) = \int_{-\infty}^{t} e^{-\tau}u(\tau)\,d\tau$.
Solution
$y(t) = (1 - e^{-t})u(t)$.
Show that compressing $x(t) = e^{-|t|}$ in time expands its bandwidth.
Solution
Compressing time by 2 doubles the bandwidth — a fundamental time-frequency trade-off.
Show that for a real signal, $|X(j\omega)|$ is even and $\angle X(j\omega)$ is odd.
Solution
For real $x(t)$: $X(-j\omega) = X^*(j\omega)$. Therefore:
Chapter 5: DT Fourier Transform
Find the DTFT of $y[n] = e^{j\pi n/4}\,x[n]$.
Solution
Find $Y(e^{j\omega})$ for $y[n] = x[n]\,(-1)^n$.
Solution
Shifts spectrum by $\pi$: converts lowpass $\leftrightarrow$ highpass.
Find the DTFT of $x[n] = 1$ for all $n$.
Solution
If $x[n] = (0.5)^n u[n]$ and $x_{(2)}[n]$ inserts zeros, find the DTFT.
Solution
Find the DTFT of $y[n] = n\,a^n u[n]$.
Solution
Using $n\,x[n] \longleftrightarrow j\,\frac{dX(e^{j\omega})}{d\omega}$:
Chapter 6: Time & Freq Characterization
Find $\tau(\omega)$ for $H(j\omega) = \frac{e^{-j3\omega}}{1+j\omega}$.
Solution
Two identical first-order lowpass filters (cutoff $\omega_c$) cascaded. Find 3dB bandwidth.
Solution
Poles at $z = 0.9e^{\pm j\pi/4}$. Where is the peak response?
Solution
Pole angle $= \pi/4$, so $|H(e^{j\omega})|$ peaks near $\omega = \pi/4$. This is a bandpass filter.
Convert $|H| = 0.01,\; 1,\; 100$ to dB.
Solution
Design a DT highpass from a lowpass $H_{lp}(e^{j\omega})$.
Solution
Or multiply impulse response by $(-1)^n$ to shift spectrum by $\pi$.
Chapter 7: Sampling
$x(t) = \cos(6000\pi t)$ sampled at 8000 samples/sec.
Solution
Why is oversampling practically useful?
Solution
Wider transition band for anti-aliasing filter (simpler analog filter). Reduces in-band quantization noise via noise shaping. Easier reconstruction.
Frequency response of DT differentiator for CT signals sampled at $1/T$.
Solution
Bandpass signal: 900–1100 Hz. Minimum sampling rate?
Solution
ZOH with $T=1$ ms. Attenuation at $f=400$ Hz?
Solution
Chapter 8: Communication Systems
4 kHz signal, PAM at 8 kHz. Minimum transmission bandwidth?
Solution
$f_c = 1$ MHz, $f_{\text{LO}} = 1.455$ MHz.
Solution
$y[n] = x[n]\cos(\pi n/4)$. Spectrum?
Solution
$y(t) = x_1\cos\omega_c t + x_2\sin\omega_c t$. Recover $x_1, x_2$.
Solution
Multiply by $\cos\omega_c t$ + LPF $\Rightarrow \frac{1}{2}x_1(t)$. Multiply by $\sin\omega_c t$ + LPF $\Rightarrow \frac{1}{2}x_2(t)$.
Works because $\cos$ and $\sin$ are orthogonal.
4 kHz audio, $f_s = 8$ kHz, 8 bits/sample.
Solution
Chapter 9: Laplace Transform
$x(t) = e^{-2t}u(t) - e^{3t}u(-t)$.
Solution
ROC includes $j\omega$ axis $\Rightarrow$ Fourier transform exists.
$X(s) = \frac{1}{s+3}$. Laplace transform of $t\,x(t)$.
Solution
Find $H(s)$ for 2nd-order Butterworth with $\omega_c=1$.
Solution
Poles at $s = \frac{-1\pm j}{\sqrt{2}}$.
$x(t) \longleftrightarrow X(s)$ with ROC $\mathcal{R}$. Find Laplace transform of $x(3t)$.
Solution
$H_1(s)=\frac{1}{s+1}$, $H_2(s)=\frac{1}{s+2}$ in parallel.
Solution
Chapter 10: z-Transform
$H(z) = \frac{z-1}{z-0.9}$. Evaluate $|H(e^{j\omega})|$ at $\omega=0$ and $\omega=\pi$.
Solution
Zero at $\omega=0$ $\Rightarrow$ highpass filter.
$H(z) = \frac{z-0.5}{(z-0.5)(z-0.8)}$.
Solution
$x[n] = n(0.5)^n u[n]$.
Solution
$H(z) = \frac{1-0.5z^{-1}}{1-0.8z^{-1}}$. Find inverse system.
Solution
Pole at $z=0.5$ (inside unit circle) $\Rightarrow$ causal inverse is stable.
$H(z) = \frac{1+z^{-1}}{(1-0.5z^{-1})(1+0.3z^{-1})}$.