Rin / Cin Measurement — High-Z Probe

Works with any oscilloscope or measurement device — no assumed scope values. R_scope is measured directly (step 1A); C_scope cancels by differential sweep (step 2).

1 Measure Rin — Resistive divider

V_gen ~ R_serie V_out R_scope GND
Two measurements, same R_serie and V_gen — only the load changes:
 • 1A: load = R_scope only  →  measures R_scope directly
 • 1B: load = R_probe ‖ R_scope  →  measures R_in_tot
R_probe = 1 / (1/R_in_tot − 1/R_scope)
No nominal scope values assumed. V_out_B < V_out_A because the probe adds parallel load.
Choose R_serie ≈ R_scope (e.g. 1 MΩ) for ~50 % attenuation and best sensitivity.

V
1A No probe — measures R_scope
Connect R_serie → scope input directly. Do not touch probe tip to anything.
Measure V_out_A at the scope input node.
V
1B With probe — measures R_in_tot
Connect probe tip to signal source. Same R_s, same V_gen.
V_out_B < V_out_A — probe in parallel reduces load impedance.
V

2 Measure Cin — Differential sweep

Two sweeps, same R_serie. C_scope + stray cancel in the subtraction.
Each R_par uses the actual load for that sweep:
2A CA = 12π · fA · Rpar_A   Rpar_A = Rserie ‖ Rscope
2B CB = 12π · fB · Rpar_B   Rpar_B = Rserie ‖ Rin_tot
Cprobe = CB − CA
Target f−3dB: 10 kHz – 300 kHz. For 1–2 pF probe: Rserie = 1 MΩ → f−3dB ≈ 10–20 kHz.

2A Sweep A — No probe (baseline)
Connect R_serie → scope input. No probe tip contact.
Sine sweep → find f_A where amplitude = 70.7 % of DC value (−3 dB).
⚠ Run step 1A first
kHz
2B Sweep B — With probe
Connect probe tip to source. Same R_s.
Sine sweep → find f_B (−3 dB). f_B < f_A — probe adds capacitance.
kHz

3 Summary & |Z_in(f)| frequency response

ParameterValueFormula / source
Complete steps 1 and 2 to see the summary.

Complete steps 1 and 2 to draw the chart.