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Impulse response of y[n] − (3/4)y[n−1] + (1/8)y[n−2] = 2x[n]

Short answer

Factor the denominator into (1−0.5e⁻ʲω)(1−0.25e⁻ʲω), use partial fractions, and apply inverse DTFT: h[n] = [4(0.5)ⁿ − 2(0.25)ⁿ] u[n].

Find impulse response for the DT system given by the following linear constant coefficient difference equation. y[n] − (3/4)y[n−1] + (1/8)y[n−2] = 2x[n]

Given: y[n]−34y[n−1]+18y[n−2]=2x[n]y[n] - \frac{3}{4}y[n-1] + \frac{1}{8}y[n-2] = 2x[n], system initially at rest.

Step 1: Frequency response

Take the DTFT (x[n−k]↔e−jωkX(ejω)x[n-k] \leftrightarrow e^{-j\omega k}X(e^{j\omega})):

(1−34e−jω+18e−j2ω)Y(ejω)=2X(ejω)\left(1 - \tfrac{3}{4}e^{-j\omega} + \tfrac{1}{8}e^{-j2\omega}\right)Y(e^{j\omega}) = 2X(e^{j\omega}) H(ejω)=21−34e−jω+18e−j2ωH(e^{j\omega}) = \frac{2}{1 - \frac{3}{4}e^{-j\omega} + \frac{1}{8}e^{-j2\omega}}

Step 2: Factorise the denominator

Let v=e−jωv = e^{-j\omega}. The roots of 1−34v+18v21 - \frac{3}{4}v + \frac{1}{8}v^2 come from p2−34p+18=0p^2 - \frac{3}{4}p + \frac{1}{8} = 0, giving p=12,14p = \frac{1}{2}, \frac{1}{4}. So

H(ejω)=2(1−12e−jω)(1−14e−jω)H(e^{j\omega}) = \frac{2}{\left(1 - \frac{1}{2}e^{-j\omega}\right)\left(1 - \frac{1}{4}e^{-j\omega}\right)}

Step 3: Partial fractions

H=A1−12v+B1−14vH = \frac{A}{1 - \frac{1}{2}v} + \frac{B}{1 - \frac{1}{4}v} A=21−14v∣v=2=21−12=4B=21−12v∣v=4=21−2=−2\begin{aligned} A &= \left.\frac{2}{1 - \frac{1}{4}v}\right|_{v=2} = \frac{2}{1 - \frac{1}{2}} = 4 \\ B &= \left.\frac{2}{1 - \frac{1}{2}v}\right|_{v=4} = \frac{2}{1 - 2} = -2 \end{aligned} H(ejω)=41−12e−jω−21−14e−jωH(e^{j\omega}) = \frac{4}{1 - \frac{1}{2}e^{-j\omega}} - \frac{2}{1 - \frac{1}{4}e^{-j\omega}}

Step 4: Inverse DTFT

Using anu[n]↔11−ae−jωa^n u[n] \leftrightarrow \frac{1}{1 - a e^{-j\omega}} (∣a∣<1|a| < 1):

h[n]=[4(12)n−2(14)n]u[n]h[n] = \left[4\left(\tfrac{1}{2}\right)^n - 2\left(\tfrac{1}{4}\right)^n\right]u[n]

Check by recursion

h[n]=2δ[n]+34h[n−1]−18h[n−2]h[n] = 2\delta[n] + \frac{3}{4}h[n-1] - \frac{1}{8}h[n-2], with h[−1]=h[−2]=0h[-1] = h[-2] = 0:

nnRecursionFormula 4(0.5)n−2(0.25)n4(0.5)^n - 2(0.25)^n
024−2=24 - 2 = 2
10.75×2=1.50.75 \times 2 = 1.52−0.5=1.52 - 0.5 = 1.5
20.75(1.5)−0.125(2)=0.8750.75(1.5) - 0.125(2) = 0.8751−0.125=0.8751 - 0.125 = 0.875
30.75(0.875)−0.125(1.5)=0.468750.75(0.875) - 0.125(1.5) = 0.468750.5−0.03125=0.468750.5 - 0.03125 = 0.46875

Both agree. Both poles (0.50.5, 0.250.25) are inside the unit circle, so the system is causal and stable; h[n]h[n] decays to zero. Also H(ej0)=21−0.75+0.125=5.333=∑h[n]=40.5−20.75H(e^{j0}) = \frac{2}{1 - 0.75 + 0.125} = 5.333 = \sum h[n] = \frac{4}{0.5} - \frac{2}{0.75}.

Answer: h[n]=[4(0.5)n−2(0.25)n]u[n]h[n] = \left[4(0.5)^n - 2(0.25)^n\right]u[n]

✓ Answer checked by Claude Opus 5.5 (high effort)

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