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Sandbox Physics

IN12 · A stable trace can be an alias

Digital Oscilloscope

When can a stable waveform be an illusion created by sampling? A stable trace can still be an alias. Different signals can pass through the same sampled values, and a trigger can align those values repeatedly. Check the sampling rate and analog bandwidth, then measure the stored samples; a smooth connecting line cannot restore changes that were never recorded.

Capture pulses and two-tone signals through a probe, analog bandwidth and ADC. Compare raw samples with their linear display and measure the same record.

Interactive modelDigital Oscilloscope

What did the sampling clock actually keep?

Saved simulated record · raw ADC acquisition

t/mst/\mathrm{ms}V/VV/\mathrm V
ADC points and linear display

Gold and violet are separate simulation references; turquoise is acquired data. Drag the pink marker to preview a new digital trigger; keeping a capture freezes its samples and standards.

Raw codes, clock and calibration provenance

First and last samples of the shown acquisition
SampleADC codet/mst/\mathrm{ms}V/VV/\mathrm VOverload

Exports retain every code, nominal timestamp, overload mask, trigger index/fraction, range, known-reference observations, version and seed. Realized jitter times are simulation provenance, not measured timestamps.

Physics tutorial

Read the samples before trusting the line

BackgroundA probe delivers a voltage to an analog input. The ADC stores one code at each clock tick, and a digital trigger chooses which part of that stream becomes a record.

Why it mattersA crisp, repeatable picture is useful only when you know which changes the instrument could capture.

Start with the essentials

Focus question
How can a stable slow wave come from a much faster input?
One-sentence intuition
Trigger alignment stabilizes a record; sampling and analog bandwidth determine what information reached it.

Core mathematical model

A declared single-pole analog input

H(f)=11+if/B,t10–90=ln⁡92πBH(f)=\frac{1}{1+\mathrm i f/B},\qquad t_{10\text{–}90}=\frac{\ln9}{2\pi B}

The rise-time relation is exact for a settled ideal step through this chosen one-pole filter. A finite pulse and sample-derived levels can give a different measured edge time.

Voltage and time come from saved standards

Vn=Vrefcn−cˉ0cˉref−cˉ0,Δt=TgfcalNgfsV_n=V_{\rm ref}\frac{c_n-\bar c_0}{\bar c_{\rm ref}-\bar c_0},\qquad \Delta t=\frac{T_g f_{\rm cal}}{N_g f_s}

Known DC levels set volts per code. A one-second reference gate and its observed tick count calibrate the common clock. Aperture jitter is not measured by that gate.

Two frequencies can have the same samples

sin⁡ ⁣(2π1100n1000)=sin⁡ ⁣(2π100n1000)\sin\!\left(2\pi\frac{1100n}{1000}\right)=\sin\!\left(2\pi\frac{100n}{1000}\right)

This equality describes ideal instantaneous samples before filtering. The full instrument also changes amplitude and phase in its analog front end.

Common difficulties

A smooth line is not extra data

Typical misconceptionIf the connecting line looks smooth, the missing fast motion has been recovered.

Better mental modelLinear interpolation passes through the stored samples and adds no independent observations between them.

Peak values can be clipped

Typical misconceptionThe largest displayed sample always gives the input peak.

Better mental modelAn overload mask marks samples outside ADC code range. A clipped peak is only a lower bound; clipped edge times are withheld.

Run the experiment

  1. 01

    Compare an edge with its samples

    Choose An edge stands still, then use Edge zoom below the apparatus.

    What to observe: The teal dots and linear display share one acquired record. Its measured rise comes from the stored 10 and 90 percent crossings.
  2. 02

    Change the sampling clock

    Choose Fast becomes slow and compare the gold input reference with the turquoise record.

    What to observe: The input is faster than the clock can distinguish. Its stable apparent period describes the sampled trace.
  3. 03

    Miss the trigger condition

    Raise the trigger level above the signal, then compare normal and auto trigger mode in the advanced controls.

    What to observe: Normal mode retains the prior capture. Auto mode keeps actual samples after its timeout, marked as untriggered.

Related experiments and articles

How physics instruments measure · Reading path

How physics instruments measure

Articles on this path that use this experiment, followed by the other experiments they suggest.

  1. ArticleWhere does the slow wave on an oscilloscope come from?
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