---
title: "Autocorrelation of cos(200πt) at τ = π/4"
subject: "Communication Systems"
chapter: 1
key: "semester_6/communication_systems:psd-esd-autocorrelation-cos200pit"
source: https://www.bctengineer.com/q/semester_6/communication_systems/psd-esd-autocorrelation-cos200pit
site: BCT Engineering
---

# Autocorrelation of cos(200πt) at τ = π/4

Communication Systems · Chapter 1: Introduction

- Asked in: 2072 Asoj (CS I), 2+3 marks
- Video: [Autocorrelation and Power Spectral Density (PSD) Examples in Digital Communications](https://www.youtube.com/watch?v=XWytSLZZP1A) — Iain Explains Signals, Systems, and Digital Comms
- Answer checked by Claude Opus 5.5 (high effort) on 2026-10-14
- Page: https://www.bctengineer.com/q/semester_6/communication_systems/psd-esd-autocorrelation-cos200pit
- Whole chapter: https://www.bctengineer.com/md/semester_6/communication_systems/chapter-1

## Question

Define power and energy spectral density function. Given a signal x(t) = cos(200πt), find the auto correlation of x(t) at τ = π/4.

## Short answer

The energy spectral density Ψ_x(f)=|X(f)|² (J/Hz) shows energy distribution for energy signals; power spectral density S_x(f)=lim_{T→∞}|X_T(f)|²/T (W/Hz) for power signals. For x(t)=cos(200πt), autocorrelation R_x(τ)=0.5 cos(200πτ). At τ=π/4, R_x≈−0.484 W.

## Answer

#### Power and energy spectral density
- **Energy spectral density (ESD):** for an energy signal, $\Psi_x(f) = |X(f)|^2$ (J/Hz); it shows how energy is distributed over frequency, and $E = \int\Psi_x(f)df$.
- **Power spectral density (PSD):** for a power signal, $S_x(f) = \lim_{T\to\infty}\frac{|X_T(f)|^2}{T}$ (W/Hz); it shows how average power is distributed over frequency, and $P = \int S_x(f)df$. Each is the Fourier transform of the corresponding autocorrelation function.

#### Autocorrelation of $x(t) = \cos(200\pi t)$ at $\tau = \pi/4$
$x(t)$ is periodic ($f_0 = 100$ Hz, $T_0 = 0.01$ s), so it is a power signal and we use the time-average autocorrelation:

$$
\begin{aligned}
R_x(\tau) &= \lim_{T\to\infty}\frac1T\int_{-T/2}^{T/2}\cos(200\pi t)\cos(200\pi(t-\tau))\,dt \\
&= \lim_{T\to\infty}\frac{1}{2T}\int_{-T/2}^{T/2}\left[\cos(200\pi\tau) + \cos(400\pi t - 200\pi\tau)\right]dt \\
&= \frac12\cos(200\pi\tau)
\end{aligned}
$$

(the second term averages to zero).

At $\tau = \pi/4$ s:

$$
\begin{aligned}
R_x\!\left(\frac{\pi}{4}\right) &= \frac12\cos\left(200\pi\cdot\frac{\pi}{4}\right) = \frac12\cos(50\pi^2) \\
&= \frac12\cos(493.48\ \text{rad}) = \frac12\times(-0.9689) \\
&\approx -0.484
\end{aligned}
$$

($493.48$ rad reduces to $493.48 - 78\times2\pi = 3.392$ rad, and $\cos 3.392 = -0.9689$.)

**Answer:** $R_x(\tau) = \frac12\cos(200\pi\tau)$, so $R_x(\pi/4) = \frac12\cos(50\pi^2) \approx -0.484$ W (normalised). For comparison $R_x(0) = 0.5$ W = average power.

## Check yourself

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

1. Which statement is right?
   A. ESD is for power signals and PSD for energy signals
   B. ESD |X(f)|^2 has unit J/Hz; PSD has unit W/Hz
   C. Both have unit W
   D. ESD is the Fourier transform of x(t)
   Answer: B. ESD (J/Hz) is for energy signals; PSD (W/Hz) is for power signals. (Key point: ESD vs PSD)

2. Why is cos(200 pi t) treated with the time-average autocorrelation?
   A. It is an energy signal
   B. It is zero for t>0
   C. It is periodic, so it is a power signal with infinite energy
   D. Its Fourier transform does not exist
   Answer: C. A sinusoid has finite power and infinite energy. (Key point: Signal type)

3. What is R_x(tau) for x(t)=cos(200 pi t)?
   A. cos(200 pi tau)
   B. (1/2) cos(200 pi tau)
   C. (1/2) cos(400 pi tau)
   D. 2 cos(200 pi tau)
   Answer: B. Using the product-to-sum identity, the double-frequency term averages to zero leaving (1/2)cos(200 pi tau). (Key point: Autocorrelation)

4. What does R_x(0) represent, and what is its value here?
   A. Average power, 0.5 W
   B. Total energy, infinity
   C. Peak amplitude, 1
   D. Bandwidth, 100 Hz
   Answer: A. R_x(0)=P=1/2 W for a unit-amplitude cosine. (Key point: Value at tau=0)

## Related in Communication Systems

- [Energy and power spectral density; spectrum analyzer](https://www.bctengineer.com/question.md?key=semester_6%2Fcommunication_systems%3Aenergy-power-spectrum-analyzer) — Communication Systems, chapter 1, asked 2×
- [ESD, PSD and autocorrelation of white noise](https://www.bctengineer.com/question.md?key=semester_6%2Fcommunication_systems%3Aesd-psd-white-noise-autocorrelation) — Communication Systems, chapter 9, asked 2×
- [Graphical auto-correlation, cross-correlation and convolution](https://www.bctengineer.com/question.md?key=semester_6%2Fcommunication_systems%3Agraphical-correlation-convolution) — Communication Systems, chapter 1
- [Autocorrelation and ESD as Fourier transform pair](https://www.bctengineer.com/question.md?key=semester_6%2Fcommunication_systems%3Aautocorrelation-esd-fourier-pair) — Communication Systems, chapter 1
- [PSD and average power of A cos(2πfct + θ)](https://www.bctengineer.com/question.md?key=semester_6%2Fcommunication_systems%3Aesd-psd-acos-power) — Communication Systems, chapter 1
- [Energy and power signal; bandwidth of a system](https://www.bctengineer.com/question.md?key=semester_6%2Fcommunication_systems%3Aenergy-power-bandwidth-system) — Communication Systems, chapter 1

## Related in other subjects

- [Energy vs power spectral density](https://www.bctengineer.com/question.md?key=semester_4%2Fsignals_and_systems%3Aenergy-vs-power-spectral-density) — Signals and Systems, chapter 3
- [Energy and power: 4sin(2πt), cos(3n/4)](https://www.bctengineer.com/question.md?key=semester_4%2Fsignals_and_systems%3Aenergy-power-4sin-cos) — Signals and Systems, chapter 1, asked 2×
- [Energy/power signals; periodicity of cos + sin](https://www.bctengineer.com/question.md?key=semester_7%2Fdigital_signal_analysis_and_processing%3Aenergy-power-periodic-2) — Digital Signal Analysis and Processing, chapter 1
- [Energy or power of DT cos(3πk/16)](https://www.bctengineer.com/question.md?key=semester_5%2Fdata_communication%3Adt-signal-cos-energy-power) — Data Communication, chapter 2
