Include measuring instruments in the circuit model
An ideal voltmeter draws no current, but a real finite input resistance is another parallel branch. An ideal ammeter adds no voltage drop, but a finite burden resistance changes the series path. This virtual packet makes both deviations explicit rather than calling a meter reading the untouched original quantity.
Learning outcome: Compare Rv=10,30,50 kΩ at zero burden, then hold Rv fixed and increase burden. Retain the original lower-resistor current separately from total current. Identify which ideal limit removes each disturbance.
Starting recap
Use charge continuity, energy per charge, consistent SI units and an explicit circuit topology. Exponential responses are supplied algebraic models; initial state, source constraint and measurement loading must be declared.
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Try
With Rv=30 kΩ and zero ammeter burden, L=30000/11 Ω. Total current is 33/13000 A≈2.53846 mA and the indicated lower voltage is 90/13≈6.92308 V, below 7.2 V. A finite series burden reduces it further.
Open the experimentPredict
The current measured upstream of both the lower resistor and voltmeter equals:
Experiment
Compare Rv=10,30,50 kΩ at zero burden, then hold Rv fixed and increase burden. Retain the original lower-resistor current separately from total current. Identify which ideal limit removes each disturbance.
Include both meters in the measured network
Worked teaching model · synthetic values · Ideal 12 V source, upper resistor 2000 ohm and lower 3000 ohm. Voltmeter is parallel to lower resistor; ammeter burden is in series with the whole divider. Both are supplied linear resistance models. No actual meter connections.
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Voltmeter loading with fixed ammeter burden
Unlike graph quantities rescale independently; read units and values, not screen angles. 1: finite-input network (solid). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for Voltmeter loading with fixed ammeter burden
finite-input network
| input resistance (kΩ) | voltage indication (V) |
|---|---|
| 10 | 6.14334 |
| 11 | 6.2069 |
| 12 | 6.26087 |
| 13 | 6.30728 |
| 14 | 6.34761 |
| 15 | 6.38298 |
| 16 | 6.41425 |
| 17 | 6.44211 |
| 18 | 6.46707 |
| 19 | 6.48956 |
| 20 | 6.50995 |
| 21 | 6.5285 |
| 22 | 6.54545 |
| 23 | 6.56101 |
| 24 | 6.57534 |
| 25 | 6.58858 |
| 26 | 6.60085 |
| 27 | 6.61224 |
| 28 | 6.62286 |
| 29 | 6.63278 |
| 30 | 6.64207 |
| 31 | 6.65077 |
| 32 | 6.65896 |
| 33 | 6.66667 |
| 34 | 6.67394 |
| 35 | 6.68081 |
| 36 | 6.68731 |
| 37 | 6.69347 |
| 38 | 6.69931 |
| 39 | 6.70487 |
| 40 | 6.71016 |
| 41 | 6.7152 |
| 42 | 6.72 |
| 43 | 6.72459 |
| 44 | 6.72897 |
| 45 | 6.73317 |
| 46 | 6.73718 |
| 47 | 6.74104 |
| 48 | 6.74473 |
| 49 | 6.74828 |
| 50 | 6.75169 |
At most 82 representative computed coordinates including endpoints; the plotted curve can use a finer grid. A table of a revealed generator is not independent measurement evidence.
| Quantity | Value | Unit |
|---|---|---|
| Uninstrumented divider voltage | 7.2 | V |
| Loaded lower equivalent resistance | 2608.7 | Ω |
| Ammeter current indication | 0.00249548 | A |
| Voltmeter voltage indication | 6.50995 | V |
| Original lower resistor current | 0.00216998 | A |
| Voltmeter current | 0.000325497 | A |
| Ammeter burden voltage | 0.499096 | V |
| Voltage measurement change | -0.690054 | V |
The meter reads the network it helps create, not an untouched ideal divider.
A voltmeter is a parallel branch; an ammeter burden adds series resistance. Infinite input resistance and zero burden are separate ideal limits. The source current includes voltmeter current, so it is not identical to the original lower-resistor current. Correcting a loading effect requires an explicit circuit model and independent meter specifications, not merely more digits.
Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.
The meter reads the network it helps create, not an untouched ideal divider.
A voltmeter is a parallel branch; an ammeter burden adds series resistance. Infinite input resistance and zero burden are separate ideal limits. The source current includes voltmeter current, so it is not identical to the original lower-resistor current. Correcting a loading effect requires an explicit circuit model and independent meter specifications, not merely more digits.
Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.
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