---
title: "Shannon-Hartley theorem; capacity limit 1.44S/N₀"
subject: "Communication Systems"
chapter: 6
key: "semester_6/communication_systems:shannon-hartley-1-44"
source: https://www.bctengineer.com/q/semester_6/communication_systems/shannon-hartley-1-44
site: BCT Engineering
---

# Shannon-Hartley theorem; capacity limit 1.44S/N₀

Communication Systems · Chapter 6: Baseband Digital Data Transmission

- Asked in: 2080 Baisakh (CS II), 6+4 marks; 2075 Asoj (CS II), 6+4 marks (asked 2 times)
- Answer checked by Claude Opus 5.5 (high effort) on 2026-10-14
- Page: https://www.bctengineer.com/q/semester_6/communication_systems/shannon-hartley-1-44
- Whole chapter: https://www.bctengineer.com/md/semester_6/communication_systems/chapter-6

## Question

Explain Shannon Hartley channel capacity theorem and its implication and theoretical limits. Show that channel capacity is 1.44S/N₀, when channel bandwidth tends to infinity.

## Short answer

Shannon-Hartley gives C = B log2(1+S/N) b/s, N=N0B; error-free transmission is possible if R<C. As B→∞, C = (S/N0) log2 e ≈ 1.44 S/N0, showing capacity saturates at a finite limit regardless of bandwidth.

## Answer

#### Shannon–Hartley theorem
The **Shannon–Hartley theorem** gives the channel capacity $C$: the highest bit rate that can be sent over a band-limited channel with additive white Gaussian noise (AWGN) with an arbitrarily small error probability.

$$
C = B \log_2\!\left(1 + \frac{S}{N}\right)\ \text{b/s}, \qquad N = N_0 B
$$

where $B$ is the bandwidth (Hz), $S$ the average signal power, and $N_0/2$ the two-sided noise power spectral density.

If the information rate $R \le C$, a coding scheme exists that makes the error probability as small as we like. If $R > C$, errors cannot be made arbitrarily small, whatever coding is used.

**Implications**
- **Bandwidth–SNR trade-off:** the same capacity can be reached with a wide band and low SNR (e.g. spread spectrum) or a narrow band and high SNR (e.g. M-ary QAM).
- Capacity grows **linearly with B** but only **logarithmically with S/N**. Doubling the power adds only about $B$ b/s at high SNR.
- It gives a benchmark: practical modems and codes (turbo, LDPC) are judged by how close they come to $C$.
- It proves that error-free communication is possible over noisy channels with proper coding. It does not say how to build the code.

**Theoretical limits**
- **Ideal system:** $R = C$. Writing $S = E_b C$:

$$
\frac{C}{B} = \log_2\!\left(1 + \frac{E_b}{N_0}\frac{C}{B}\right) \Rightarrow \frac{E_b}{N_0} = \frac{2^{C/B} - 1}{C/B}
$$

- As $C/B \to 0$ (infinite bandwidth), $E_b/N_0 \to \ln 2 = 0.693$, i.e. **−1.6 dB**. This is the **Shannon limit**: below it, no error-free transmission is possible at any bandwidth.
- Increasing bandwidth alone cannot give unlimited capacity, because noise power $N_0 B$ also grows (shown below).

#### Capacity with infinite bandwidth
$$
C = B \log_2\!\left(1 + \frac{S}{N_0 B}\right)
$$

Let $x = \dfrac{S}{N_0 B}$, so $B = \dfrac{S}{N_0 x}$. As $B \to \infty$, $x \to 0$:

$$
\begin{aligned}
C &= \frac{S}{N_0} \cdot \frac{1}{x} \log_2(1 + x) = \frac{S}{N_0} \log_2 (1+x)^{1/x} \\
C_\infty &= \lim_{x \to 0} \frac{S}{N_0} \log_2 (1+x)^{1/x} = \frac{S}{N_0} \log_2 e \\
&= \frac{S}{N_0} \times 1.4427 \approx 1.44 \frac{S}{N_0}
\end{aligned}
$$

using $\lim_{x \to 0} (1+x)^{1/x} = e$ and $\log_2 e = 1/\ln 2 = 1.4427$.

So even with infinite bandwidth, the capacity stays finite at $C_\infty \approx 1.44\, S/N_0$ b/s. Capacity can be raised only by raising the signal power or lowering the noise density.

## Check yourself

The answer's key points as multiple-choice questions, with the correct option and why.

1. What does the Shannon-Hartley formula C = B log2(1 + S/N) give?
   A. The minimum bit rate of a channel
   B. The highest rate with arbitrarily small error over a band-limited AWGN channel
   C. The average error probability
   D. The bandwidth needed for any code
   Answer: B. If R <= C, suitable coding gives arbitrarily small error probability; if R > C it cannot. (Key point: Capacity formula)

2. What is the capacity as B tends to infinity?
   A. Infinite
   B. Zero
   C. 1.44 S/N0, which is finite
   D. 0.693 S/N0
   Answer: C. C_inf = (S/N0) log2 e = 1.44 S/N0, because noise power N0 B grows with B. (Key point: Infinite bandwidth)

3. Which limit is used in deriving C_inf = 1.44 S/N0?
   A. lim x->0 (1 + x)^(1/x) = e
   B. lim x->inf (1 + x)^x = 1
   C. lim x->0 sin(x)/x = 0
   D. lim x->inf log2 x = 0
   Answer: A. With x = S/(N0 B), C = (S/N0) log2 (1 + x)^(1/x), which tends to (S/N0) log2 e. (Key point: Derivation step)

4. What is the Shannon limit on Eb/N0 for reliable communication?
   A. ln 2 = 0.693, i.e. -1.6 dB
   B. 1.44, i.e. 1.6 dB
   C. 0 dB exactly
   D. 3 dB
   Answer: A. As C/B tends to 0, Eb/N0 tends to ln 2, about -1.6 dB; below it, no error-free transmission is possible. (Key point: Shannon limit)

## Related in Communication Systems

- [Shannon channel capacity theorem and its implication](https://www.bctengineer.com/question.md?key=semester_6%2Fcommunication_systems%3Ashannon-capacity-implication) — Communication Systems, chapter 6
- [Entropy and information rate; Shannon limit as bandwidth → ∞](https://www.bctengineer.com/question.md?key=semester_6%2Fcommunication_systems%3Aentropy-info-rate-shannon-limit) — Communication Systems, chapter 6
- [Shannon channel capacity theorem and its limitations](https://www.bctengineer.com/question.md?key=semester_6%2Fcommunication_systems%3Ashannon-capacity-limitations) — Communication Systems, chapter 6, asked 2×
- [Shannon-Hartley theorem; energy/power of e^(−2t)u(t)](https://www.bctengineer.com/question.md?key=semester_6%2Fcommunication_systems%3Ashannon-hartley-energy-e2t) — Communication Systems, chapter 1
- [Implications and limitations of Shannon-Hartley theorem](https://www.bctengineer.com/question.md?key=semester_6%2Fcommunication_systems%3Ashannon-hartley-implications-limits) — Communication Systems, chapter 6
- [Information and entropy; capacity as bandwidth → ∞](https://www.bctengineer.com/question.md?key=semester_6%2Fcommunication_systems%3Ainformation-entropy-capacity-infinite) — Communication Systems, chapter 6

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