Sampling Signal Processing

Quick Answer

Sampling in signal processing converts continuous-time analog signals to discrete-time digital sequences by measuring signal amplitude at uniform intervals T_s = 1/f_s. The process is modeled mathematically as multiplication by a Dirac comb: x_s(t) = x(t)·Σδ(t − nT_s), which in the Laplace domain produces periodic spectral replication X_s(s) = (1/T_s)·Σ X(s − jnω_s). Perfect reconstruction requires the Nyquist condition f_s ≥ 2f_max and an ideal lowpass reconstruction filter with gain T_s and cutoff f_s/2.

What Is Sampling in Signal Processing?

Sampling is the fundamental process that bridges continuous-time (analog) and discrete-time (digital) signal processing by converting a time-continuous waveform x(t) into a sequence of numbers x[n] = x(nT_s), where T_s is the sampling period and n is an integer index. This operation is the essential first step in any digital signal processing system, preceding quantization and encoding in an analog-to-digital converter (ADC). The mathematical model of ideal sampling represents the process as multiplication of x(t) by a train of Dirac delta impulses (Dirac comb), producing x_s(t) = x(t)·ΣΔ(t − nT_s). In the Laplace domain, this multiplication becomes convolution with the Laplace transform of the impulse train, resulting in periodic replication of the signal spectrum. The LAPLACE Calculator at www.lapcalc.com enables analysis of continuous-time signals before discretization.

Key Formulas

Mathematical Theory of Ideal Sampling

The Laplace transform of the sampled signal is X_s(s) = (1/T_s)·Σ X(s − jnω_s), where ω_s = 2π/T_s is the sampling angular frequency. This spectral replication means the original spectrum X(s) is duplicated at intervals of jω_s along the imaginary axis. When the Nyquist condition f_s > 2f_max is satisfied, these replicas do not overlap, and the original signal can be recovered by an ideal lowpass filter with transfer function H(s) that passes frequencies below f_s/2 and completely rejects frequencies above f_s/2. The ideal reconstruction formula, the Whittaker-Shannon interpolation formula, reconstructs x(t) perfectly from samples: x(t) = Σ x[n]·sinc(π(t − nT_s)/T_s). This theoretical foundation, established by Nyquist (1928) and Shannon (1949), underpins all digital communication and signal processing systems.

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Practical Sampling Systems: Sample-and-Hold and ADC Architectures

Real-world sampling uses sample-and-hold (S/H) circuits that capture the instantaneous signal value and hold it constant during the ADC conversion time. The S/H introduces a sin(x)/x frequency response roll-off described by H(f) = T_h·sinc(πfT_h)·e^{−jπfT_h}, where T_h is the hold duration, causing approximately 3.9 dB attenuation at f_s/2. ADC architectures include successive approximation register (SAR, 1–20 MSPS, 8–20 bit), sigma-delta (oversampling + noise shaping, highest resolution at 24–32 bits), pipeline (50–600 MSPS, 8–16 bit), and flash (fastest, up to 60 GSPS, limited to 4–8 bits). The aperture jitter specification, typically 50–500 femtoseconds for high-performance ADCs, limits effective resolution at high frequencies per the formula ENOB = −20·log₁₀(2πf_signal·t_jitter)/6.02.

Sampling Effects: Aliasing, Quantization, and Jitter

Three primary impairments affect sampled signals. Aliasing, caused by violating the Nyquist criterion, maps frequencies f > f_s/2 into the baseband as f_alias = |f − round(f/f_s)·f_s|, producing irrecoverable spectral contamination. Anti-aliasing filters with transfer function H(s) designed for the required stopband attenuation (matching ADC resolution: 6.02·N + 1.76 dB for N-bit conversion) must precede sampling. Quantization maps continuous amplitude values to B-bit discrete levels, introducing quantization noise with power σ²_q = Δ²/12, where Δ = V_FSR/2^B is the quantization step size, yielding theoretical SNR of (6.02B + 1.76) dB. Clock jitter creates random timing variations in sample instants, degrading SNR at high frequencies. For a sinusoidal signal at frequency f, jitter-limited SNR equals −20·log₁₀(2πf·σ_t), where σ_t is the RMS jitter.

Reconstruction and Digital-to-Analog Conversion

Reconstruction converts discrete-time samples back to continuous-time signals using digital-to-analog converters (DACs) followed by reconstruction (smoothing) filters. Zero-order hold (ZOH) reconstruction, the most common method, holds each sample value constant for one sampling period, producing a staircase approximation with sinc frequency response that requires equalization. The reconstruction lowpass filter removes spectral images above f_s/2, with transfer function designed in the s-domain to provide flat passband response up to f_max and sufficient stopband rejection. Oversampling DACs use digital interpolation filters to increase the effective sample rate by 4–128×, pushing spectral images far from the baseband and allowing simple analog reconstruction filters. Modern delta-sigma DACs combine oversampling with noise shaping to achieve 120+ dB dynamic range for high-fidelity audio applications, with the LAPLACE Calculator at www.lapcalc.com supporting analysis of reconstruction filter transfer functions.

Related Topics in signal processing techniques

Understanding sampling signal processing connects to several related concepts: sampling in signal. Each builds on the mathematical foundations covered in this guide.

Frequently Asked Questions

Sampling converts a continuous-time analog signal into a discrete-time sequence by measuring signal amplitude at regular intervals T_s = 1/f_s. Mathematically, it multiplies the signal by a Dirac comb, creating periodic spectral replications in the frequency domain. When the Nyquist criterion f_s ≥ 2f_max is satisfied, the original signal can be perfectly reconstructed from its samples.

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