Updated 2026-08-21 · one desk, one shelf, no climate control
Every number on this site came off one of these. I list the specifications
because a measurement without its instrument's limits is an opinion, and because three of the
six write-ups here turned on a limit rather than on a fault.
I deliberately do not name manufacturers or model numbers. What decides whether a
measurement is admissible is the sample rate, the analogue bandwidth and the threshold
behaviour, not the badge on the front panel.
CAN pairs, RS-485 pairs, ground-to-ground potential
single-ended millivolt work
Bench supply
0–30 V, 0–3 A, current limit settable to 10 mA
finding shorts before they find the board, sink-current tests
transient load response
Isolated DC-DC bricks
5 V in, 5 V out, 1 W, 2.5 kV isolation
separating a remote transceiver from its local ground
anything above a few tens of milliamps
Resistor and capacitor decade boxes
1 Ω–100 kΩ in 1 Ω steps; 10 pF–1 µF
sweeping pull-up values without a soldering iron
high-frequency substitution, the leads dominate
Probing habits that changed my results
Ground spring instead of the ground lead. The crocodile lead on a scope
probe adds enough inductance to invent overshoot. On the CAN work it fabricated a 600 mV
ringing artefact that disappeared the moment I used a spring tip. If a waveform shows ringing,
re-probe before you believe it.
Trigger on the thing you doubt, not on the clock. Framing errors are rare
events; triggering on chip select or on a start edge and letting it sit for a few minutes
catches more than a thousand screenshots of healthy traffic.
Record the capture settings in the same file as the capture. Sample rate,
threshold, probe attenuation. I lost an entire session's worth of credibility once because I
could not say afterwards whether a run had been at 24 MS/s or at 8.
Measure the same quantity a second way. The SPI mismatch was proved by
reading the same register over the sensor's other interface. One instrument agreeing with itself
is not corroboration.
What I do not have, and what that costs
No frequency counter or calibrated reference
This is why the baud-rate measurement ends with an
unresolved 0.5 % discrepancy. I can measure a ratio between two signals on the bench; I cannot
tell you the absolute frequency of either to better than my analyser's quantisation.
No time-domain reflectometer
Cable impedance and velocity factor are taken from the cable's published figures rather than
measured. On the 95 m CAN segment I used 5 ns/m as given, and said so in the post.
No climate chamber
Everything here is at room temperature, roughly 21 °C. Crystal drift over temperature, which
matters a great deal for baud-rate budgets in the field, is therefore outside what I can
demonstrate.
Only two analogue channels
I cannot show you a differential pair and its chip select simultaneously with analogue
fidelity. Where a post needed both, the two captures were taken separately on the same trigger
condition, which is weaker evidence and is flagged where it happens.