---
title: "Matched filter approximation using ideal LPF"
subject: "Communication Systems"
chapter: 9
key: "semester_6/communication_systems:matched-filter-ideal-lpf"
source: https://www.bctengineer.com/q/semester_6/communication_systems/matched-filter-ideal-lpf
site: BCT Engineering
---

# Matched filter approximation using ideal LPF

Communication Systems · Chapter 9: Noise in Communication Systems

- Asked in: 2070 Chaitra (CS II), 6 marks
- Answer checked by Claude Opus 5.5 (high effort) on 2026-10-14
- Page: https://www.bctengineer.com/q/semester_6/communication_systems/matched-filter-ideal-lpf
- Whole chapter: https://www.bctengineer.com/md/semester_6/communication_systems/chapter-9

## Question

Explain the approximation of the matched filter for a rectangular pulse using an Ideal low pass filter with variable bandwidth.

## Short answer

An ideal LPF with variable bandwidth approximates the matched filter for a rectangular pulse. Optimum bandwidth B ≈ 0.685/T yields output SNR ratio ρ ≈0.825 compared to the matched filter, only about0.84 dB degradation.

## Answer

The true matched filter for a rectangular pulse is an integrate-and-dump filter, giving $(S/N)_{max} = 2E/N_0$. A simpler practical receiver uses an **ideal LPF** whose bandwidth $B$ can be chosen; the question is how close it can come.

**Set-up.** Pulse $p(t) = A$ for $|t| \le T/2$ (energy $E = A^2T$), white noise PSD $N_0/2$, ideal LPF of unit gain and bandwidth $B$. Pulse spectrum:

$$
P(f) = AT\,\frac{\sin \pi fT}{\pi fT}
$$

```text
 |H(f)|
   1 +-----------+
     |           |
 ----+-----+-----+-----> f
    -B     0     B
```

**Peak output signal** (at the pulse centre $t=0$):

$$
\begin{aligned}
s_o(0) &= \int_{-B}^{B} AT\frac{\sin\pi fT}{\pi fT}\,df = \frac{2A}{\pi}\int_0^{\pi BT}\frac{\sin x}{x}\,dx \\
&= \frac{2A}{\pi}\,\text{Si}(\pi BT)
\end{aligned}
$$

**Output noise power:** $N_o = \dfrac{N_0}{2}\cdot 2B = N_0B$

**Output SNR**

$$
\left(\frac{S}{N}\right)_{LPF} = \frac{4A^2\,\text{Si}^2(\pi BT)}{\pi^2N_0B}
$$

**Compare with the matched filter**, $(S/N)_{MF} = 2A^2T/N_0$:

$$
\rho = \frac{(S/N)_{LPF}}{(S/N)_{MF}} = \frac{2\,\text{Si}^2(\pi BT)}{\pi^2\,BT}
$$

**Effect of bandwidth**

- $B$ too small: pulse energy is cut off, peak signal is small.
- $B$ too large: little extra signal but noise grows in proportion to $B$.
- An optimum exists in between.

Evaluating $\rho$ numerically:

| $BT$ | 0.5 | 0.685 | 1.0 | 1.5 |
|---|---|---|---|---|
| $\rho$ | 0.762 | 0.825 | 0.695 | 0.349 |

**Result:** the best choice is $B \approx 0.685/T$ (about $0.7/T$), giving $\rho \approx 0.825$, i.e. only about **0.84 dB** worse than the true matched filter. Hence an ideal LPF with bandwidth about $0.7 \times$ the bit rate is a good, simple approximation to the matched filter for rectangular pulses.

## Check yourself

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

1. Why is an ideal LPF used to approximate the matched filter for a rectangular pulse?
   A. It gives higher SNR than the matched filter
   B. It is a simpler practical receiver whose bandwidth B can be chosen
   C. It removes all noise
   D. It needs no knowledge of the pulse
   Answer: B. The true matched filter is integrate-and-dump; the LPF is simpler and the question is how close it gets by choosing B. (Key point: Why an LPF approximation)

2. What happens if the LPF bandwidth B is made too large?
   A. Peak signal drops sharply
   B. Little extra signal is gained but noise grows in proportion to B
   C. Noise power falls
   D. The pulse energy is cut off
   Answer: B. Noise power is N_0 B, so it keeps increasing while the peak signal saturates. (Key point: Bandwidth trade-off)

3. The best LPF bandwidth for a rectangular pulse of width T is about
   A. 0.2/T
   B. 0.7/T
   C. 1.5/T
   D. 3/T
   Answer: B. The ratio rho is maximum (about 0.825) at BT of about 0.685. (Key point: Optimum bandwidth)

4. At the optimum bandwidth, the ideal LPF output SNR is about what fraction of the matched filter SNR?
   A. 0.825, about 0.84 dB worse
   B. 0.5, about 3 dB worse
   C. 0.95, about 0.2 dB worse
   D. 1.0, no loss
   Answer: A. rho is about 0.825 at BT = 0.685, which is roughly a 0.84 dB loss. (Key point: Loss relative to matched filter)

## Close variants set in other exams

- [Matched filter approximation using RC low pass filter](https://www.bctengineer.com/question.md?key=semester_6%2Fcommunication_systems%3Amatched-filter-rc-approximation) — Communication Systems, chapter 9, asked 2×

## Related in Communication Systems

- [Noise equivalent bandwidth of RC low pass filter](https://www.bctengineer.com/question.md?key=semester_6%2Fcommunication_systems%3Aneb-rc-lowpass) — Communication Systems, chapter 9
- [Noise equivalent bandwidth; matched filter is time reversed](https://www.bctengineer.com/question.md?key=semester_6%2Fcommunication_systems%3Aneb-matched-filter-reverse) — Communication Systems, chapter 9
- [Moments of random variable; NEB of RC-LPF; output noise power](https://www.bctengineer.com/question.md?key=semester_6%2Fcommunication_systems%3Amoments-neb-rc-lpf) — Communication Systems, chapter 9

## Related in other subjects

- [Impulse response of ideal low pass filter](https://www.bctengineer.com/question.md?key=semester_4%2Fsignals_and_systems%3Aideal-lpf-impulse-response) — Signals and Systems, chapter 5, asked 5×
- [Impulse response of DT ideal low pass filter](https://www.bctengineer.com/question.md?key=semester_4%2Fsignals_and_systems%3Aideal-lpf-discrete-time) — Signals and Systems, chapter 6
- [Ideal low pass and high pass filters](https://www.bctengineer.com/question.md?key=semester_4%2Fsignals_and_systems%3Afrequency-response-lp-hp-filters) — Signals and Systems, chapter 5
- [Ideal band pass and low pass filters (DT)](https://www.bctengineer.com/question.md?key=semester_4%2Fsignals_and_systems%3Aideal-bandpass-lowpass-dt) — Signals and Systems, chapter 6
