The capacity of band-limited additive white Gaussian Noise (AWGN) channel is given by \(C = W{\log _2}\left[ {1 + \frac{P}{{{\sigma ^2}w}}} \right]\) bits per second (bps), where W is the channel Bandwidth, P is the average power received and σ2 is the one-sided power spectral density of the AWGN. For a fixed \(\frac{P}{{{\sigma ^2}}} = 1000\), the channel capacity (in kbps) with infinite Bandwidth (W → ∞) is approximately
1.44
The question asks us to find the channel capacity of a band-limited Additive White Gaussian Noise (AWGN) channel when the bandwidth (W) approaches infinity. We are given the formula for channel capacity and a specific ratio of power to noise spectral density.
The capacity of a band-limited AWGN channel is given by the Shannon-Hartley theorem:
\[C = W{\log _2}\left[ {1 + \frac{P}{{{\sigma ^2}W}}} \right]\text{ bits per second (bps)}\]
Where:
We are provided with the following information:
First, substitute the given ratio \(\frac{P}{{{\sigma ^2}}} = 1000\) into the capacity formula:
\[C = W{\log _2}\left[ {1 + \frac{1000}{W}} \right]\]
Now, we need to evaluate the limit of this expression as \(W \to \infty\):
\[C_{\text{infinite bandwidth}} = \lim_{W \to \infty} W{\log _2}\left[ {1 + \frac{1000}{W}} \right]\]
To solve this limit, we can use a standard limit property related to the mathematical constant 'e'. Recall that \(\lim_{x \to 0} \frac{\ln(1+x)}{x} = 1\).
Let's rewrite the \(\log_2\) term in terms of natural logarithm (\(\ln\)):
We know that \({\log _b}a = \frac{{{\log _c}a}}{{{\log _c}b}}\), so \({\log _2}x = \frac{{\ln x}}{{\ln 2}}\).
Applying this to our capacity formula:
\[C = W \frac{\ln\left(1 + \frac{1000}{W}\right)}{\ln 2}\]
Rearrange the terms to fit the limit form:
\[C = \frac{1}{\ln 2} \times \frac{\ln\left(1 + \frac{1000}{W}\right)}{\frac{1}{W}}\]
Multiply the numerator and denominator inside the fraction by 1000 to match the form \(\frac{\ln(1+x)}{x}\), where \(x = \frac{1000}{W}\):
\[C = \frac{1000}{\ln 2} \times \frac{\ln\left(1 + \frac{1000}{W}\right)}{\frac{1000}{W}}\]
As \(W \to \infty\), let \(x = \frac{1000}{W}\). Then \(x \to 0\). The limit becomes:
\[C_{\text{infinite bandwidth}} = \lim_{x \to 0} \frac{1000}{\ln 2} \times \frac{\ln(1+x)}{x}\]
Since \(\lim_{x \to 0} \frac{\ln(1+x)}{x} = 1\), the expression simplifies to:
\[C_{\text{infinite bandwidth}} = \frac{1000}{\ln 2} \times 1\]
Now, we need to calculate the numerical value. We know that \(\ln 2 \approx 0.6931\).
\[C_{\text{infinite bandwidth}} \approx \frac{1000}{0.6931}\]
\[C_{\text{infinite bandwidth}} \approx 1442.66\text{ bps}\]
The question asks for the channel capacity in kilobits per second (kbps). To convert bps to kbps, we divide by 1000:
\[C_{\text{kbps}} = \frac{1442.66}{1000}\text{ kbps}\]
\[C_{\text{kbps}} \approx 1.44266\text{ kbps}\]
Rounding to two decimal places, the channel capacity is approximately 1.44 kbps.
Based on our calculation, the channel capacity with infinite bandwidth for the given conditions is approximately 1.44 kbps.
Noise factor of a system is defined as:
Match List I with List II:
| List I | List II | ||
| (A) | Shannon's theorem | (I) | Capacity of Gaussian Noise channel |
| (B) | Shannon-Hartley theorem | (II) | Rate of Information |
| (C) | Bayes theorem | (III) | Energy of a signal |
| (D) | Parseval's theorem | (IV) | Conditional probabilities |
Choose the correct answer from the options given below:
The information capacity (bits/sec) of a channel with bandwidth C and transmission time T is given by
Consider an additive white Gaussian noise (AWGN) channel with bandwidth W and noise power spectral density $\frac{N_0}{2}$. Let $P_{av}$ denote the average transmit power constraint. Which one of the following plots illustrates the dependence of the channel capacity C on the bandwidth W (keeping $P_{av}$ and $N_0$ fixed)?
A voice-grade AWGN (additive white Gaussian noise) telephone channel has a bandwidth of 4.0 kHz and two-sided noise power spectral density $ \frac{\eta}{2} = 2.5\times10^{-5} $ Watt per Hz. If information at the rate of 52 kbps is to be transmitted over this channel with arbitrarily small bit error rate, then the minimum bit-energy $E_b$ (in mJ/bit) necessary is ____________