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Shannon-Hartley theorem; energy/power of e^(−2t)u(t)

With a suitable example explain Shannon-Hartley channel capacity theorem. Determine whether the given signal x(t) = e^(−2t)u(t) is a power or an energy signal.

Shannon–Hartley channel capacity theorem

The theorem gives the maximum error-free data rate (channel capacity) of a band-limited channel disturbed by additive white Gaussian noise (AWGN):

C=Blog⁡2(1+SN) bit/sC = B\log_2\left(1 + \frac{S}{N}\right) \ \text{bit/s}

where BB = channel bandwidth (Hz), SS = average signal power, N=N0BN = N_0B = noise power in the band.

Meaning:

  • If the information rate R≤CR \le C, there exists a coding scheme that makes the error probability as small as desired.
  • If R>CR > C, error-free transmission is impossible whatever coding is used.
  • Bandwidth and SNR can be traded: the same capacity can be obtained with less bandwidth and more power, or vice versa.
  • As B→∞B \to \infty, capacity does not become infinite; it approaches C∞=1.44 S/N0C_\infty = 1.44\,S/N_0.

Example: a telephone channel with B=3.1B = 3.1 kHz and SNR =30= 30 dB (S/N=1000S/N = 1000):

C=3100log⁡2(1+1000)=3100×9.967≈30.9 kbit/sC = 3100\log_2(1 + 1000) = 3100 \times 9.967 \approx 30.9\ \text{kbit/s}

So no modem can reliably send more than about 30.9 kbit/s over such a line.

Is x(t)=e−2tu(t)x(t) = e^{-2t}u(t) an energy or power signal?

Energy:

E=∫−∞∞∣x(t)∣2 dt=∫0∞e−4t dt=[e−4t−4]0∞=0−(−14)=14 J\begin{aligned} E &= \int_{-\infty}^{\infty} |x(t)|^2\,dt = \int_{0}^{\infty} e^{-4t}\,dt \\ &= \left[\frac{e^{-4t}}{-4}\right]_0^{\infty} = 0 - \left(-\frac14\right) = \frac14\ \text{J} \end{aligned}

Power:

P=lim⁡T→∞1T∫0T/2e−4t dt=lim⁡T→∞1−e−2T4T=0P = \lim_{T\to\infty}\frac{1}{T}\int_{0}^{T/2} e^{-4t}\,dt = \lim_{T\to\infty}\frac{1 - e^{-2T}}{4T} = 0

Answer: Energy E=0.25E = 0.25 J (finite, non-zero) and power P=0P = 0, so x(t)=e−2tu(t)x(t) = e^{-2t}u(t) is an energy signal.

✓ Answer checked by Claude Opus 5.5 (high effort)

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