Transmission line & reflections
Explore a signal as it propagates, reflects, and settles at the receiver.
Step: 0 → A; other signals: ±A. Random rate is in Mbit/s. Time and voltage scales stay fixed when excitation changes.
50 Ω matching & bounce behavior
Matching is about controlling what happens when a traveling wave reaches an impedance discontinuity. The schematic and lattice share the same parameters.
Step: 0 → A; other signals: ±A. Random rate is in Mbit/s. Time and voltage scales stay fixed when excitation changes.
Differential signals & skew
The pair is useful because equal and opposite fields cancel. Spacing changes field sharing; skew breaks simultaneity and converts differential energy into common mode.
Differential Vpp sets the full bipolar swing; step excursion is Vpp/2. Shape and rate are shared.
Crosstalk & coupling
The aggressor does not “send noise through air.” Its changing electric and magnetic fields share geometry with the victim. Reference-plane distance and parallelism control that overlap.
Step: 0 → A; other signals: ±A. Random rate is in Mbit/s. Time and voltage scales stay fixed when excitation changes.
Via transition & return geometry
A signal via is only half of a transition. The return current also needs a low-inductance path between reference structures. Remove it and the loop area expands.
Stackup geometry drives Z₀
Characteristic impedance emerges from field geometry. Width, plane spacing, copper thickness, and dielectric constant all redistribute electric and magnetic energy.
Audit the channel you just built
This page does not teach new rules. It evaluates the state created across the other labs and turns the visual experiments into engineering review questions.