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Signals and Systems•Unit 1• EEE2006

Signal Classifications, Mathematical Operations & System Properties

Continuous and discrete signal types, elementary waveforms (Dirac impulse, unit step, ramp, complex exponential, sinc), independent variable transformations (time shifting, time scaling, time reversal), orthogonal even and odd signal decomposition, signal energy and power calculations, and rigorous classification of systems across linearity, time invariance, causality, BIBO stability, memory, and invertibility.

Learning Mode Filter (#29):Personalize View
Skills Built:Continuous vs Discrete Time Representation (x(t) vs x[n])Singularity Function Calculus (δ(t), u(t), r(t), rect, tri, sinc)Dirac Delta Sifting (∫ x(t)δ(t - t₀)dt = x(t₀)) & Scaling PropertiesIndependent Variable Transformations: x(at - b) = x(a(t - b/a))Orthogonal Even/Odd Decomposition (xe(t), xo(t)) & Energy ConservationEnergy (0 < E < ∞, P = 0) vs Power (E = ∞, 0 < P < ∞) TaxonomyLinearity & Superposition Axiom Proof (Additivity + Homogeneity)Time-Invariance Shift Commutation Test (𝓣{x(t - t₀)} = y(t - t₀))Causality, Dynamic Memory, BIBO Stability & Invertibility Verification

1. 5 Key Ideas: Signal Architecture & System Axioms

Idea 1: Continuous vs Discrete Signals & The Elementary Singularity Toolkit

In electrical and computer engineering, a signal is a mathematical function of one or more independent variables that conveys information about the state or behavior of a physical system:

  • Continuous-Time (CT) Signals x(t)x(t): The independent variable tt is continuous over the real numbers (t∈Rt \in \mathbb{R}). Examples: analog voltages, acoustic pressure, ambient temperature.
  • Discrete-Time (DT) Signals x[n]x[n]: The independent variable nn is defined strictly at integer indices (n∈Zn \in \mathbb{Z}). Represented as indexed sequences x[n]x[n], typically obtained by sampling a continuous signal at uniform intervals TsT_s: x[n]=x(nTs)x[n] = x(n T_s).

Engineering signal analysis relies on a foundational set of elementary building blocks:

  1. Unit Step Function (Heaviside Function): u(t)={1,t>00,t<0andu[n]={1,n≥00,n<0u(t) = \begin{cases} 1, & t > 0 \\ 0, & t < 0 \end{cases} \quad \text{and} \quad u[n] = \begin{cases} 1, & n \ge 0 \\ 0, & n < 0 \end{cases} Models instantaneous switching on of a circuit or DC voltage excitation.

  2. Dirac Delta Function (Unit Impulse): The continuous unit impulse δ(t)\delta(t) is a generalized function (distribution) defined by its integral properties rather than instantaneous point values: δ(t)=0for t≠0,∫−∞∞δ(t) dt=1\delta(t) = 0 \quad \text{for } t \ne 0, \quad \int_{-\infty}^{\infty} \delta(t)\,dt = 1 It is the formal distributional derivative of the unit step function: δ(t)=du(t)dt  ⟺  u(t)=∫−∞tδ(τ) dτ\delta(t) = \frac{du(t)}{dt} \iff u(t) = \int_{-\infty}^{t} \delta(\tau)\,d\tau In discrete time, the unit impulse δ[n]\delta[n] (Kronecker delta) is simply: δ[n]={1,n=00,n≠0\delta[n] = \begin{cases} 1, & n = 0 \\ 0, & n \ne 0 \end{cases}

  3. Unit Ramp Function r(t)r(t): r(t)=∫−∞tu(τ) dτ=t⋅u(t)={t,t≥00,t<0r(t) = \int_{-\infty}^{t} u(\tau)\,d\tau = t \cdot u(t) = \begin{cases} t, & t \ge 0 \\ 0, & t < 0 \end{cases}

  4. Standard Pulse Geometries:

    • Rectangular Pulse: rect(tT)=u(t+T2)−u(t−T2)\text{rect}\left(\frac{t}{T}\right) = u\left(t + \frac{T}{2}\right) - u\left(t - \frac{T}{2}\right) (unit height, width TT, centered at origin).
    • Triangular Pulse: Λ(tT)=(1−∣t∣T)rect(t2T)\Lambda\left(\frac{t}{T}\right) = \left(1 - \frac{|t|}{T}\right) \text{rect}\left(\frac{t}{2T}\right) (base 2T2T, peak height 1 at t=0t=0).
    • Normalized Sinc Pulse: sinc(t)=sin⁡(πt)πt\text{sinc}(t) = \frac{\sin(\pi t)}{\pi t} (zero crossings at all non-zero integers t=±1,±2,…t = \pm 1, \pm 2, \dots).

Idea 2: Sifting, Sampling & Distributional Calculus of the Dirac Delta

The Dirac delta impulse possesses powerful analytical properties essential for convolution, Fourier analysis, and sampling theory:

  1. Sampling / Multiplication Property: Multiplying any continuous function x(t)x(t) by an impulse concentrated at t=t0t = t_0 isolates the value x(t0)x(t_0): x(t) δ(t−t0)=x(t0) δ(t−t0)x(t)\,\delta(t - t_0) = x(t_0)\,\delta(t - t_0)

  2. Sifting (Filtering) Property: Integrating the product of x(t)x(t) and δ(t−t0)\delta(t - t_0) extracts the scalar value of x(t)x(t) at the impulse singularity: ∫−∞∞x(t) δ(t−t0) dt=x(t0)\int_{-\infty}^{\infty} x(t)\,\delta(t - t_0)\,dt = x(t_0) Proof: ∫−∞∞x(t)δ(t−t0)dt=∫−∞∞x(t0)δ(t−t0)dt=x(t0)∫−∞∞δ(t−t0)dt=x(t0)⋅1=x(t0)\int_{-\infty}^\infty x(t)\delta(t - t_0)dt = \int_{-\infty}^\infty x(t_0)\delta(t - t_0)dt = x(t_0) \int_{-\infty}^\infty \delta(t - t_0)dt = x(t_0) \cdot 1 = x(t_0).

  3. Time-Scaling Property of Impulses: For any non-zero real constant a≠0a \ne 0: δ(at)=1∣a∣δ(t)andδ(at−b)=1∣a∣δ(t−ba)\delta(at) = \frac{1}{|a|} \delta(t) \quad \text{and} \quad \delta(at - b) = \frac{1}{|a|} \delta\left(t - \frac{b}{a}\right) Notice the absolute value: compressing an impulse by factor aa magnifies its integral intensity by 1/∣a∣1/|a|, and reflection δ(−t)=δ(t)\delta(-t) = \delta(t) confirms that the impulse is an even function.

  4. Derivative of the Impulse (Doublet): The unit doublet δ′(t)=dδ(t)dt\delta'(t) = \frac{d\delta(t)}{dt} satisfies the derivative sifting property: ∫−∞∞x(t) δ′(t−t0) dt=−x′(t0)\int_{-\infty}^{\infty} x(t)\,\delta'(t - t_0)\,dt = -x'(t_0)

Idea 3: Mathematical Operations on Independent Variables & Order Precedence

Modifying a signal's independent time axis is fundamental to radar ranging, audio pitch shifting, and communication modulation. Three primary elementary operations exist:

  1. Time Shifting: y(t)=x(t−t0)y(t) = x(t - t_0)
    • If t0>0t_0 > 0: Time Delay — the waveform shifts to the RIGHT by t0t_0 seconds.
    • If t0<0t_0 < 0: Time Advance — the waveform shifts to the LEFT by ∣t0∣|t_0| seconds.
  2. Time Scaling: y(t)=x(at)y(t) = x(at) (a>0a > 0)
    • If a>1a > 1: Time Compression — the waveform speeds up and shrinks horizontally by factor aa.
    • If 0<a<10 < a < 1: Time Expansion — the waveform slows down and stretches horizontally by factor 1/a1/a.
  3. Time Reversal (Reflection): y(t)=x(−t)y(t) = x(-t)
    • Flips the waveform horizontally around the vertical axis t=0t = 0.

The Combined Transformation Trap: x(at−b)x(at - b)

A common source of errors in exams is plotting a combined transformation y(t)=x(at−b)y(t) = x(at - b).

Method 1 (Factored Form — Shift First, Then Scale): Factor out the scaling coefficient aa: y(t)=x(a(t−ba))y(t) = x\left(a\left(t - \frac{b}{a}\right)\right)

  • Step 1: Shift x(t)x(t) by ba\frac{b}{a} (to the right if b/a>0b/a > 0).
  • Step 2: Scale by aa (and reflect if a<0a < 0).

Method 2 (Scale First, Then Shift): Write directly as x(at−b)x(at - b):

  • Step 1: Scale x(t)x(t) to obtain x(at)x(at).
  • Step 2: Replace tt with t−bat - \frac{b}{a}! Notice: Shifting x(at)x(at) by bb yields x(a(t−b))=x(at−ab)x(a(t - b)) = x(at - ab), NOT x(at−b)x(at - b)! To obtain x(at−b)x(at - b) after scaling, you must shift by ba\frac{b}{a}, not bb.

Idea 4: Orthogonal Even & Odd Decomposition and Energy Conservation

Every real continuous or discrete signal x(t)x(t) can be uniquely decomposed into the sum of an even component xe(t)x_e(t) and an odd component xo(t)x_o(t): x(t)=xe(t)+xo(t)x(t) = x_e(t) + x_o(t)

Where:

  • Even Component xe(t)x_e(t): Symmetric about the vertical axis (xe(−t)=xe(t)x_e(-t) = x_e(t)): xe(t)=x(t)+x(−t)2x_e(t) = \frac{x(t) + x(-t)}{2}
  • Odd Component xo(t)x_o(t): Antisymmetric through the origin (xo(−t)=−xo(t)x_o(-t) = -x_o(t)): xo(t)=x(t)−x(−t)2x_o(t) = \frac{x(t) - x(-t)}{2}

Fundamental Properties of Even & Odd Signals

  1. xo(0)=0x_o(0) = 0 for any continuous odd signal (since xo(0)=−xo(0)  ⟹  2xo(0)=0x_o(0) = -x_o(0) \implies 2x_o(0) = 0).
  2. xe(0)=x(0)x_e(0) = x(0).
  3. The integral of any odd function over symmetric limits is identically zero: ∫−AAxo(t) dt=0\int_{-A}^{A} x_o(t)\,dt = 0
  4. Product Rules:
    • Even×Even=Even\text{Even} \times \text{Even} = \text{Even}
    • Odd×Odd=Even\text{Odd} \times \text{Odd} = \text{Even}
    • Even×Odd=Odd\text{Even} \times \text{Odd} = \text{Odd}
  5. Orthogonality & Energy Conservation: Even and odd functions are mutually orthogonal: ∫−∞∞xe(t)xo(t) dt=0\int_{-\infty}^{\infty} x_e(t) x_o(t)\,dt = 0 Consequently, the total energy of x(t)x(t) is the direct sum of the energies of its even and odd parts: Ex=Exe+ExoE_x = E_{x_e} + E_{x_o}

Idea 5: Energy vs Power Taxonomy & The 6 Foundational System Axioms

Energy vs Power Signal Classification

The instantaneous power dissipated across a normalized 1-Ω1\text{-}\Omega resistor by voltage or current x(t)x(t) is p(t)=∣x(t)∣2p(t) = |x(t)|^2.

  • Total Signal Energy (EE): E=∫−∞∞∣x(t)∣2 dt(CT)andE=∑n=−∞∞∣x[n]∣2(DT)E = \int_{-\infty}^{\infty} |x(t)|^2\,dt \quad \text{(CT)} \quad \text{and} \quad E = \sum_{n=-\infty}^{\infty} |x[n]|^2 \quad \text{(DT)}
  • Average Signal Power (PP): P=lim⁡T→∞12T∫−TT∣x(t)∣2 dt(CT)andP=lim⁡N→∞12N+1∑n=−NN∣x[n]∣2(DT)P = \lim_{T \to \infty} \frac{1}{2T} \int_{-T}^{T} |x(t)|^2\,dt \quad \text{(CT)} \quad \text{and} \quad P = \lim_{N \to \infty} \frac{1}{2N + 1} \sum_{n=-N}^{N} |x[n]|^2 \quad \text{(DT)}

The Three Mutually Exclusive Classes:

  1. Energy Signal: 0<E<∞  ⟹  P=00 < E < \infty \implies P = 0. (Finite-duration pulses, decaying exponentials e−atu(t)e^{-at}u(t)).
  2. Power Signal: 0<P<∞  ⟹  E=∞0 < P < \infty \implies E = \infty. (Periodic waveforms, sine waves, square waves, unit step u(t)u(t)).
  3. Neither Energy Nor Power Signal: E=∞E = \infty and P=∞P = \infty. (Ramp functions r(t)=tr(t) = t, growing exponentials eatu(t)e^{at}u(t)).

The 6 Core System Axioms

A system is a mathematical operator T\mathcal{T} that transforms an input signal x(t)x(t) into an output signal y(t)=T{x(t)}y(t) = \mathcal{T}\{x(t)\}:

  1. Linearity: The system satisfies the Principle of Superposition (both Additivity and Homogeneity): T{ax1(t)+bx2(t)}=aT{x1(t)}+bT{x2(t)}=ay1(t)+by2(t)\mathcal{T}\{a x_1(t) + b x_2(t)\} = a \mathcal{T}\{x_1(t)\} + b \mathcal{T}\{x_2(t)\} = a y_1(t) + b y_2(t) Necessary check: Zero input must produce zero output (x=0  ⟹  y=0x=0 \implies y=0). Any non-zero DC bias (e.g., y=2x+3y = 2x + 3) makes a system non-linear!
  2. Time-Invariance: A time delay in the input produces an identical time delay in the output: If T{x(t)}=y(t),then T{x(t−t0)}=y(t−t0)\text{If } \mathcal{T}\{x(t)\} = y(t), \quad \text{then } \mathcal{T}\{x(t - t_0)\} = y(t - t_0) A system is time-variant if time tt appears explicitly outside the input signal argument (e.g., y(t)=t⋅x(t)y(t) = t \cdot x(t) or y(t)=x(2t)y(t) = x(2t)).
  3. Causality: The output y(t)y(t) at any instant t=t0t = t_0 depends only on current and past input values (x(t)x(t) for t≤t0t \le t_0), never on future inputs (t>t0t > t_0). (All real-time physical systems are causal).
  4. BIBO Stability: Every Bounded Input produces a Bounded Output: ∣x(t)∣≤Mx<∞  ⟹  ∣y(t)∣≤My<∞for all t|x(t)| \le M_x < \infty \implies |y(t)| \le M_y < \infty \quad \text{for all } t
  5. Memory (Static vs Dynamic):
    • Memoryless (Static): Output y(t)y(t) at any instant tt depends strictly and exclusively on the input x(t)x(t) at that exact same instant tt (e.g., y(t)=R⋅i(t)y(t) = R \cdot i(t)).
    • Dynamic (With Memory): Output depends on past or future inputs (e.g., capacitors v(t)=1C∫−∞ti(τ)dτv(t) = \frac{1}{C}\int_{-\infty}^t i(\tau)d\tau, delays y(t)=x(t−1)y(t) = x(t - 1)).
  6. Invertibility: Distinct inputs produce distinct outputs. An inverse system T−1\mathcal{T}^{-1} exists such that T−1{T{x(t)}}=x(t)\mathcal{T}^{-1}\{\mathcal{T}\{x(t)\}\} = x(t). (Systems like y(t)=x2(t)y(t) = x^2(t) or y(t)=0y(t) = 0 are non-invertible).

2. Key Formula Box

Formula & Unit Quick-Reference Strip
Even ComponentSI

Symmetric component satisfying xe(-t) = xe(t) and xe(0) = x(0).

Odd ComponentSI

Antisymmetric component satisfying xo(-t) = -xo(t) and xo(0) = 0.

Total Signal EnergySI

Integral of squared magnitude across normalized 1-ohm resistance (Joules).

Average Signal PowerSI

Time-averaged energy rate over infinite horizon (Watts); for periodic signals P = (1/T0) ∫ |x|² dt.

Impulse Sifting PropertySI

Convolution identity isolating instantaneous signal amplitude at singularity coordinate t0.

Impulse Scaling LawSI

Compression scaling relationship with absolute value preserving total unit area.

Superposition AxiomSI

Linearity definition requiring simultaneous additivity and homogeneity.


3. In-Depth Mathematical Derivations

Derivation 1: Rigorous Proof of the Sifting Property via Limiting Gaussian Distribution

Why does the Dirac delta extract x(t0)x(t_0) under integration?

Derivation 2: Orthogonal Energy Decomposition Ex=Exe+ExoE_x = E_{x_e} + E_{x_o}

Why is the cross product of even and odd functions identically zero?

Derivation 3: Average Power of a Sinusoid x(t)=Acos⁡(ω0t+θ)x(t) = A\cos(\omega_0 t + \theta)

Why is the average power of a sinusoid equal to A2/2A^2/2, independent of frequency and phase?


4. Typical Laboratory Hardware Values & Engineering Benchmarks

Typical Laboratory Hardware Ranges
Parameter / PartTypical ValueLab RangePractical Notes
ECG Signal Voltage Amplitude1.0 mV peak0.5 - 4.0 mVDifferential biopotential; classified as an energy-like transient pulse train requiring low-noise instrumentation amplifiers.
Audio Dynamic Range (Power Ratio)96 dB (16-bit PCM)60 - 120 dBPower ratio of 10^(9.6) ≈ 4 × 10^9 between loudest unclipped signal and background quantization noise.
Standard Radar Chirp Pulse EnergyE ≈ 10 - 50 Joules1 - 500 JHigh peak power (e.g. 50 kW) over narrow pulse width (e.g. 1 ms) yielding finite energy per pulse.
DSP Sampling Clock Jittert_jitter < 50 ps10 - 200 psUnintended time shifts t - (n Ts + tjitter) degrade high-frequency ADC SNR via noise = 20 log10(1 / [2π f tjitter]).
Analog Group Delay Distortionτg ≤ 2.5 μs1 - 10 μsNon-constant group delay dφ/dω causes dispersion, stretching and distorting transformed waveforms x(at - b).

5. Worked Examples: Step-by-Step Analytical Solutions

Step-by-Step Worked Problem

[Graphical Transformation Problem] Given a triangular continuous pulse x(t) defined by: x(t) = t + 1 for -1 ≤ t ≤ 0, x(t) = 1 - t for 0 ≤ t ≤ 1, and x(t) = 0 elsewhere. Sketch and define the mathematical equation for the transformed signal y(t) = 2 x(3 - 2t).

Step 1: Put the argument into standard factored form
y(t) = 2 x(3 - 2t) = 2 x(-2t + 3) = 2 x(-2(t - 1.5)). Here: Amplitude scaling: A = 2 Time scaling: a = -2 (meaning reflection + compression by 2x) Time shift: t0 = +1.5 (shift to the right by 1.5 seconds).
Step 2: Map the critical boundary points using the argument relationship
Let tau = 3 - 2t => t = (3 - tau) / 2. Original critical points of x(tau): 1. Left corner: tau = -1 => t = (3 - (-1)) / 2 = 4 / 2 = 2.0 s. 2. Peak apex: tau = 0 => t = (3 - 0) / 2 = 1.5 s. 3. Right corner: tau = +1 => t = (3 - 1) / 2 = 2 / 2 = 1.0 s.
Step 3: Determine new time interval and amplitude
The transformed signal is non-zero strictly on the interval [1.0, 2.0]. Notice that the original left corner (tau = -1) mapped to t = 2.0 (reversal), and original right corner (tau = 1) mapped to t = 1.0. Peak amplitude at apex t = 1.5 s is 2 * (1) = 2.0.
Step 4: Formulate the piecewise linear equation for y(t)
For 1.0 <= t <= 1.5: Slope = (2 - 0) / (1.5 - 1.0) = 2 / 0.5 = +4. y(t) = 4(t - 1.0) = 4t - 4. For 1.5 <= t <= 2.0: Slope = (0 - 2) / (2.0 - 1.5) = -2 / 0.5 = -4. y(t) = -4(t - 2.0) = 8 - 4t. y(t) = 0 for t < 1.0 and t > 2.0.
Step-by-Step Worked Problem

[Even/Odd Decomposition & Energy Conservation] A one-sided exponential signal is given by x(t) = e^(-2t) u(t). (1) Find the algebraic expressions for its even part xe(t) and odd part xo(t), and (2) Calculate the total energy Ex of the signal and prove that Ex = Exe + Exo.

Step 1: Write expressions for x(t) and reversed signal x(-t)
x(t) = e^(-2t) u(t). x(-t) = e^(+2t) u(-t).
Step 2: Formulate Even and Odd Components
Even component: x_e(t) = 0.5 [e^(-2t) u(t) + e^(2t) u(-t)] = 0.5 e^(-2|t|) for all t in (-∞, ∞). Odd component: x_o(t) = 0.5 [e^(-2t) u(t) - e^(2t) u(-t)] = 0.5 sgn(t) e^(-2|t|).
Step 3: Compute Total Energy Ex
E_x = ∫_{-\infty}^{\infty} |x(t)|^2 dt = ∫_{0}^{\infty} [e^(-2t)]^2 dt = ∫_{0}^{\infty} e^(-4t) dt = [-e^(-4t) / 4]_{0}^{\infty} = 0 - (-1/4) = 1/4 = 0.250 Joules.
Step 4: Compute Even Component Energy Exe
Because x_e(t) is symmetric: E_xe = 2 ∫_{0}^{\infty} [0.5 e^(-2t)]^2 dt = 2 * 0.25 ∫_{0}^{\infty} e^(-4t) dt = 0.5 * (1/4) = 1/8 = 0.125 Joules.
Step 5: Compute Odd Component Energy Exo
Because x_o(t) is antisymmetric: E_xo = 2 ∫_{0}^{\infty} [0.5 e^(-2t)]^2 dt = 2 * 0.25 ∫_{0}^{\infty} e^(-4t) dt = 0.5 * (1/4) = 1/8 = 0.125 Joules. Sum: E_xe + E_xo = 0.125 + 0.125 = 0.250 J = E_x! Proven.
Step-by-Step Worked Problem

[6-Axiom System Verification] A continuous system is described by the input-output equation y(t) = x(t/3) + 2. Determine whether the system is: (1) Linear, (2) Time-Invariant, (3) Causal, (4) BIBO Stable, (5) Memoryless, and (6) Invertible. Justify each answer mathematically.

Step 1: Test Linearity (Superposition Principle)
Check zero input: x(t) = 0 => y(t) = 0/3 + 2 = 2 != 0. A linear system MUST have zero output for zero input. Furthermore: T{a x1 + b x2} = a x1(t/3) + b x2(t/3) + 2. a T{x1} + b T{x2} = a[x1(t/3) + 2] + b[x2(t/3) + 2] = a x1(t/3) + b x2(t/3) + 2(a + b). Since 2 != 2(a + b) for arbitrary scalars, the system is NON-LINEAR.
Step 2: Test Time-Invariance (Shift Commutativity)
Let input be delayed by t0: x_d(t) = x(t - t0). System response to x_d(t): y1(t) = x_d(t/3) + 2 = x(t/3 - t0) + 2. Now delay original output by t0: y(t - t0) = x((t - t0)/3) + 2 = x(t/3 - t0/3) + 2. Since x(t/3 - t0) != x(t/3 - t0/3), y1(t) != y(t - t0). Therefore, the system is TIME-VARIANT.
Step 3: Test Causality
Consider negative time t = -3: y(-3) = x(-3/3) + 2 = x(-1) + 2. Here present time is t = -3, but the system depends on input at t = -1 (which is in the FUTURE relative to -3)! Because output depends on future inputs for t < 0, the system is NON-CAUSAL.
Step 4: Test BIBO Stability
Let |x(t)| <= M < ∞ for all t. Then |y(t)| = |x(t/3) + 2| <= |x(t/3)| + 2 <= M + 2 < ∞. Since a bounded input always yields a bounded output, the system is BIBO STABLE.
Step 5: Test Memory (Static vs Dynamic)
At t = 3, y(3) depends on x(1), which is a past input relative to t = 3. Because output depends on inputs at times other than present instant t, the system is DYNAMIC (HAS MEMORY).
Step 6: Test Invertibility
Solve for x(t) in terms of y(t): y(t) = x(t/3) + 2 => x(t/3) = y(t) - 2. Replacing t with 3t: x(t) = y(3t) - 2. A unique inverse system exists. Therefore, the system is INVERTIBLE.

6. Common Exam Traps & Where Marks Are Lost

Common Exam Traps & Where Marks Are Lost

Avoid these classic calculation errors frequently spotted on semester examination answer scripts:

  • Transformation Order Misapplication: When graphing y(t) = x(2t - 4), students frequently scale first and shift by 4 units right. Remember: x(2t - 4) = x(2(t - 2)). The true time shift is 2 units to the right, NOT 4! Scaling first by 2 and then shifting by 4 creates x(2(t - 4)) = x(2t - 8), which is completely wrong.
  • Zero-Input Linearity Check: Never spend 10 minutes performing lengthy superposition algebra on an affine system like y(t) = 3x(t) + 5. Immediately evaluate x = 0: if y(0) ≠ 0, the system is instantly non-linear! State this in one line to save valuable exam time.
  • Time Reversal in Causality: A system defined by y(t) = x(-t) is frequently mistaken for causal. For any negative time (e.g. t = -2), y(-2) = x(+2). At t = -2, t = +2 is 4 seconds into the future! Hence, time reversal is ALWAYS non-causal for continuous signals.
  • Impulse Scaling Coefficient Loss: When evaluating ∫_{-∞}^∞ x(t) δ(3t - 6) dt, remember to apply the scaling property δ(3t - 6) = δ(3(t - 2)) = (1/3) δ(t - 2). The integral evaluates to (1/3) x(2), NOT x(2). Forgetting the 1/|a| factor is a classic trap.
  • Energy vs Power Mutual Exclusivity: If you compute E = 12 J for a signal, its power is AUTOMATICALLY P = 0 W. Do not write P = 12 W! If a signal has finite non-zero energy, spreading that energy across infinite time t → ∞ yields zero average power.

7. Interactive Circuit Verification & Laboratory Workbench

Experiment with signal transformations (delay, scale, reversal), observe orthogonal even and odd waveform slices, classify energy vs power signals, and evaluate the 6 system axioms in the live simulator below:

Interactive Engineering Simulator
signal-operations

Simulator will mount when scrolled into view (conserving CPU & memory)

Try Breaking It: Predict Before You Test

Can a physical, real-time audio delay line be time-invariant and causal if its delay time fluctuates with temperature: y(t) = x(t - t₀(t))?


8. Parametric Practice Problem

Parametrised Practice Problem

Thévenin Equivalent of a Loaded Voltage Divider

A 12 V DC voltage source powers a divider with R1 = 30 Ω and R2 = 80 Ω. Calculate the open-circuit Thévenin voltage V_th (in Volts) appearing across terminals of R2.

V
Progressive Hints:

9. Unit Mastery Quiz

5-Question Mastery Check

Unit Quiz: Signal Classifications, Operations & System Properties

Q1.What is the value of the definite integral ∫_{-∞}^{∞} (t³ + 4t + 2) · δ(t - 3) dt?

Q2.If x(t) is an arbitrary signal of total energy Ex = 10 J, what is the value of the cross-correlation integral ∫_{-∞}^{∞} xe(t) xo(t) dt between its even and odd components?

Q3.A signal is defined as x(t) = 5 cos(100πt) + 3 sin(200πt). How is this signal classified?

Q4.Consider the system described by y(t) = x(t) · cos(10t). Which of the following statements is TRUE?

Q5.What is the even part xe(t) of the unit step function u(t)?

Q6.Why is an ideal differentiator y(t) = dx(t)/dt considered a dynamic system with memory in continuous time?

0 of 6 answered

10. References & Further Reading

  1. Oppenheim, Alan V., Alan S. Willsky, and S. Hamid Nawab: Signals and Systems, 2nd Edition, Prentice Hall (Chapter 1: Signals and Systems).
  2. Proakis, John G., and Dimitris G. Manolakis: Digital Signal Processing: Principles, Algorithms, and Applications, 4th Edition, Pearson.
  3. Haykin, Simon, and Barry Van Veen: Signals and Systems, 2nd Edition, John Wiley & Sons.
  4. Lathi, Bhagwandas P.: Linear Systems and Signals, 2nd Edition, Oxford University Press.
  5. Presidency University Courseware: EEE2006 - Signals and Systems, Department of Electrical & Electronics Engineering, Bengaluru.