Sampling at the Nyquist Rate
August 1, 2019
Sampling
Frequency Domain Consequences of Sampling
Reconstruction Via Interpolation
Quantization noise and over-sampling
Differential Quantization / Delta Modulation
Noise Shaping / Delta-Sigma Modulation
Back to: Sampling & Reconstruction
In Example 1, the time waveform x(t) was sampled at π₯s = 4 Γ πΏh. The resulting DTFT spectral images were spread out in the DTFT frequency domain.
By examining these results, it is apparent that the minimum sample rate is π₯s = 2 Γ πΏh. Anything less would result in the overlap of spectral images.
The π₯s = 2Β Γ πΏh rate is called the Nyquist rate. Example 5 is similar to Example 4, but the sample rate π₯s is reduced to the Nyquist rate.
Frequency Content of a Waveform Sampled at Nyquist Rate (Ex. 5)
Given the time waveform illustrated in Figure 2.1:
(1) ![Rendered by QuickLaTeX.com \begin{equation*} x(t)=\frac{1}{\sqrt{2\pi}}\left[\frac{\sin(t/2)}{t/2}\right]^2 \triangleq \frac{1}{\sqrt{2\pi}}sinc^2\left(\frac{t}{2}\right) \end{equation*}](https://vru.vibrationresearch.com/wp-content/ql-cache/quicklatex.com-c87be8fc3ce4df4c31c27b000c5246b5_l3.png)
The Fourier transform π·Μ(π) is the triangle function illustrated in Figure 2.3 with the highest frequency component of πΏh = 1/2π Hz.
The waveform x(t) sampled at π₯s β 2 Γ πΏh = 4 Γ 1/2π = 1/π gives a sample period of π = 1/π₯s = π and is illustrated in Figure 2.5.

Figure 2.5. Sample sequence.
Using this sample rate and Theorem 1, a DTFT πΈΜ(π) of y(n) is expressed as:
(2) ![]()
(3) ![Rendered by QuickLaTeX.com \begin{equation*} =\frac{\sqrt{2\pi}}{\pi}\sum_{n\in\mathbb{Z}}\tilde{X}\left(\frac{1}{\pi}[\omega-2\pi n]\right) \end{equation*}](https://vru.vibrationresearch.com/wp-content/ql-cache/quicklatex.com-e78191df6d795edbbe6edb355b743672_l3.png)
Conclusion
- π·Μ(π) repeats every 2π (this is true of all DTFTs)
- π·Μ(π) reaches 0 when (1/π) π = 1 or π = π
- The height of each triangle is
or about 0.798 (see Figures 2.6 and 2.7)

Figure 2.6. Fourier transform.

Figure 2.7. DTFT.