The input \(x(t)\) and output \(y(t)\) of a system are related by
Equation
\[y(t) = \int_{-\infty}^{t} x(\tau)\cos(3\tau)\,d\tau.\]
The system is:
- time-invariant and stable
- stable and not time-invariant
- time-invariant and not stable
- not time-invariant and not stable
Solution
Time-invariance: for a shifted input \(x(t-t_0)\), substituting \(\tau'=\tau-t_0\) gives
Equation
\[y'(t) = \int_{-\infty}^{t-t_0} x(\tau')\cos\big[3(\tau'+t_0)\big]\,d\tau' \ne y(t-t_0),\]
because the explicit \(\cos(3\tau)\) factor is not shifted. The system is not time-invariant.
Stability: take the bounded input \(x(t)=\cos(3t)\). Then \(x(\tau)\cos(3\tau)=\cos^2(3\tau)=\tfrac{1}{2}\big(1+\cos 6\tau\big)\), and
Equation
\[y(t) = \int_{-\infty}^{t}\tfrac{1}{2}\big(1+\cos 6\tau\big)\,d\tau \to \infty \quad\text{as } t\to\infty,\]
so a bounded input yields an unbounded output. The system is not stable.
Note: this paper's draft key marked (B). The worked analysis above shows the system is neither time-invariant nor stable, so the correct choice is (D), which is also the official answer.
D
Final Answer
Correct answer: D.
The Fourier transform of a signal \(h(t)\) is \(H(j\omega)=2\cos(\omega)\dfrac{\sin(2\omega)}{\omega}\). The value of \(h(0)\) is:
- \(\tfrac{1}{4}\)
- \(\tfrac{1}{2}\)
- \(1\)
- \(2\)
Solution
Write \(\cos\omega = \tfrac{1}{2}(e^{j\omega}+e^{-j\omega})\) and let \(X(\omega)=\dfrac{2\sin 2\omega}{\omega}\), which is the transform of the rectangular pulse \(x(t)=1\) for \(-2
Equation
\[H(j\omega) = \tfrac{1}{2}\big[e^{j\omega}X(\omega) + e^{-j\omega}X(\omega)\big] \;\Longleftrightarrow\; h(t) = \tfrac{1}{2}\big[x(t+1)+x(t-1)\big].\]
Therefore \(h(0) = \tfrac{1}{2}\big[x(1)+x(-1)\big] = \tfrac{1}{2}(1+1) = 1\).
C
Final Answer
Correct answer: C.
Consider \(\dfrac{d^2y}{dt^2} + 2\dfrac{dy}{dt} + y = \delta(t)\) with \(y(0^-)=-2\) and \(\left.\tfrac{dy}{dt}\right|_{0^-}=0\). Find \(\left.\dfrac{dy}{dt}\right|_{0^+}\).
- \(-2\)
- \(-1\)
- \(0\)
- \(1\)
Solution
Taking the Laplace transform with the given initial conditions:
Equation
\[Y(s)(s^2+2s+1) - (s)(-2) - 0 - 2(-2) = 1 \;\Rightarrow\; Y(s) = \frac{-2s-3}{(s+1)^2} = \frac{-2}{s+1} - \frac{1}{(s+1)^2}.\]
Inverting, \(y(t) = -2e^{-t} - t e^{-t}\), so
Equation
\[\frac{dy}{dt} = e^{-t} + t e^{-t}, \qquad \left.\frac{dy}{dt}\right|_{0^+} = 1.\]
D
Final Answer
Correct answer: D.
Let \(y[n]\) be the convolution of \(h[n]=\left(\tfrac{1}{2}\right)^n u[n]\) and a causal sequence \(g[n]\). If \(y[0]=1\) and \(y[1]=\tfrac{1}{2}\), then \(g[1]\) equals:
- \(0\)
- \(\tfrac{1}{2}\)
- \(1\)
- \(\tfrac{3}{2}\)
Solution
With \(h[0]=1,\ h[1]=\tfrac{1}{2}\) and \(g[n]=0\) for \(n<0\):
Equation
\[y[0] = g[0]h[0] = g[0] = 1.\]
Equation
\[y[1] = g[0]h[1] + g[1]h[0] = 1\cdot\tfrac{1}{2} + g[1] = \tfrac{1}{2} \;\Rightarrow\; g[1] = 0.\]
A
Final Answer
Correct answer: A.
The unilateral Laplace transform of \(f(t)\) is \(F(s)=\dfrac{1}{s^2+s+1}\). The transform of \(t\,f(t)\) is:
- \(-\dfrac{s}{(s^2+s+1)^2}\)
- \(-\dfrac{2s+1}{(s^2+s+1)^2}\)
- \(\dfrac{s}{(s^2+s+1)^2}\)
- \(\dfrac{2s+1}{(s^2+s+1)^2}\)
Solution
By the frequency-differentiation property \(\mathcal{L}\{t f(t)\} = -\dfrac{d}{ds}F(s)\):
Equation
\[\mathcal{L}\{t f(t)\} = -\frac{d}{ds}\left(\frac{1}{s^2+s+1}\right) = \frac{2s+1}{(s^2+s+1)^2}.\]
D
Final Answer
Correct answer: D.
If \(x[n]=\left(\tfrac{1}{3}\right)^{|n|} - \left(\tfrac{1}{2}\right)^n u[n]\), the region of convergence of its Z-transform is:
- \(\tfrac{1}{3}<|z|<3\)
- \(\tfrac{1}{3}<|z|<\tfrac{1}{2}\)
- \(\tfrac{1}{2}<|z|<3\)
- \(|z|>\tfrac{1}{3}\)
Solution
The two-sided term \(\left(\tfrac{1}{3}\right)^{|n|}\) splits into a causal part (ROC \(|z|>\tfrac{1}{3}\)) and an anti-causal part (ROC \(|z|<3\)), giving \(\tfrac{1}{3}<|z|<3\). The second term \(\left(\tfrac{1}{2}\right)^n u[n]\) has ROC \(|z|>\tfrac{1}{2}\). The overall ROC is the intersection:
Equation
\[\Big(\tfrac{1}{3}<|z|<3\Big)\cap\Big(|z|>\tfrac{1}{2}\Big) = \tfrac{1}{2}<|z|<3.\]
C
Final Answer
Correct answer: C.