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Convolution integral; e^(−t)u(t) * e^(−2t)u(t−3)

Short answer

Convolution integral is y(t)=∫x(τ)h(t−τ)dτ. For x(t)=e^{-t}u(t) and y(t)=e^{-2t}u(t−3), overlap is 0≤τ≤t−3 for t≥3, giving z(t)=(e^{-(t+3)}−e^{-2t})u(t−3).

Derive formula to calculate convolution integral for continuous time LTI system. Find convolution between following continuous time signals x(t) = e^(−t)u(t) and y(t) = e^(−2t)u(t−3)

Derivation of the convolution integral

The convolution integral gives the output y(t)y(t) of a continuous-time LTI system for any input x(t)x(t), once the impulse response h(t)h(t) is known.

Step 1 – Represent the input by impulses (sifting property):

x(t)=∫−∞∞x(τ) δ(t−τ) dτx(t) = \int_{-\infty}^{\infty} x(\tau)\,\delta(t-\tau)\,d\tau

So x(t)x(t) is a continuous sum of shifted impulses δ(t−τ)\delta(t-\tau), each weighted by x(τ) dτx(\tau)\,d\tau.

Step 2 – Response to one impulse: by definition, δ(t)→h(t)\delta(t) \rightarrow h(t).

Step 3 – Time invariance: δ(t−τ)→h(t−τ)\delta(t-\tau) \rightarrow h(t-\tau).

Step 4 – Linearity (homogeneity): x(τ) δ(t−τ) dτ→x(τ) h(t−τ) dτx(\tau)\,\delta(t-\tau)\,d\tau \rightarrow x(\tau)\,h(t-\tau)\,d\tau.

Step 5 – Linearity (additivity): adding (integrating) the responses to all the weighted impulses,

y(t)=∫−∞∞x(τ) h(t−τ) dτ=x(t)∗h(t)y(t) = \int_{-\infty}^{\infty} x(\tau)\,h(t-\tau)\,d\tau = x(t) * h(t)

This is the convolution integral. By changing the variable λ=t−τ\lambda = t-\tau it can also be written y(t)=∫−∞∞h(τ) x(t−τ) dτy(t)=\int_{-\infty}^{\infty} h(\tau)\,x(t-\tau)\,d\tau.

Graphical steps: (1) change tt to τ\tau; (2) fold h(τ)h(\tau) to get h(−τ)h(-\tau); (3) shift by tt to get h(t−τ)h(t-\tau); (4) multiply by x(τ)x(\tau); (5) integrate over the overlap; (6) repeat for all tt.

Convolution of x(t)=e−tu(t)x(t)=e^{-t}u(t) and y(t)=e−2tu(t−3)y(t)=e^{-2t}u(t-3)

Let z(t)=x(t)∗y(t)z(t) = x(t) * y(t):

z(t)=∫−∞∞e−τu(τ)  e−2(t−τ)u(t−τ−3) dτz(t) = \int_{-\infty}^{\infty} e^{-\tau}u(\tau)\; e^{-2(t-\tau)}u(t-\tau-3)\,d\tau

Limits:

  • u(τ)=1u(\tau) = 1 only for τ≥0\tau \ge 0.
  • u(t−τ−3)=1u(t-\tau-3) = 1 only for τ≤t−3\tau \le t-3.

So the product is non-zero only for 0≤τ≤t−30 \le \tau \le t-3, which needs t≥3t \ge 3.

Case 1: t<3t < 3 – no overlap, so z(t)=0z(t) = 0.

Case 2: t≥3t \ge 3:

z(t)=∫0t−3e−τ e−2t e2τ dτ=e−2t∫0t−3eτ dτ=e−2t[eτ]0t−3=e−2t(et−3−1)=e−(t+3)−e−2t\begin{aligned} z(t) &= \int_{0}^{t-3} e^{-\tau}\,e^{-2t}\,e^{2\tau}\,d\tau \\ &= e^{-2t}\int_{0}^{t-3} e^{\tau}\,d\tau \\ &= e^{-2t}\left[e^{\tau}\right]_0^{t-3} \\ &= e^{-2t}\left(e^{t-3} - 1\right) \\ &= e^{-(t+3)} - e^{-2t} \end{aligned}

Check: at t=3t = 3, z(3)=e−6−e−6=0z(3) = e^{-6} - e^{-6} = 0, so the output starts smoothly from zero. At t=4t = 4, z(4)=e−7−e−8≈0.000576z(4) = e^{-7} - e^{-8} \approx 0.000576.

Answer:

z(t)=x(t)∗y(t)=(e−(t+3)−e−2t)u(t−3)z(t) = x(t)*y(t) = \left(e^{-(t+3)} - e^{-2t}\right)u(t-3)

Shortcut check: e−2tu(t−3)=e−6 e−2(t−3)u(t−3)e^{-2t}u(t-3) = e^{-6}\,e^{-2(t-3)}u(t-3), so it is e−6e^{-6} times e−2tu(t)e^{-2t}u(t) delayed by 3. Since e−tu(t)∗e−2tu(t)=(e−t−e−2t)u(t)e^{-t}u(t) * e^{-2t}u(t) = (e^{-t}-e^{-2t})u(t), the result is e−6(e−(t−3)−e−2(t−3))u(t−3)=(e−(t+3)−e−2t)u(t−3)e^{-6}\left(e^{-(t-3)} - e^{-2(t-3)}\right)u(t-3) = \left(e^{-(t+3)} - e^{-2t}\right)u(t-3), the same answer.

✓ Answer checked by Claude Opus 5.5 (high effort)

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