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SCIENCE · INVESTIGATE AND EXPLAIN

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 experiment

Predict

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.

Reset keeps your prediction, captures and practice history.

Voltmeter loading with fixed ammeter burden

voltage indication (V)input resistance (kΩ)0506.751690

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)
106.14334
116.2069
126.26087
136.30728
146.34761
156.38298
166.41425
176.44211
186.46707
196.48956
206.50995
216.5285
226.54545
236.56101
246.57534
256.58858
266.60085
276.61224
286.62286
296.63278
306.64207
316.65077
326.65896
336.66667
346.67394
356.68081
366.68731
376.69347
386.69931
396.70487
406.71016
416.7152
426.72
436.72459
446.72897
456.73317
466.73718
476.74104
486.74473
496.74828
506.75169

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.

Calculated quantities under the declared measurement model
QuantityValueUnit
Uninstrumented divider voltage7.2V
Loaded lower equivalent resistance2608.7Ω
Ammeter current indication0.00249548A
Voltmeter voltage indication6.50995V
Original lower resistor current0.00216998A
Voltmeter current0.000325497A
Ammeter burden voltage0.499096V
Voltage measurement change-0.690054V

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.

Understand

Define topology, recipient and initial conditions

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.

Derive the quantitative response

The uninstrumented divider has 2000 Ω above and 3000 Ω below a 12 V source, so its lower voltage is 12×3000/5000=7.2 V. A voltmeter resistance Rv across the lower resistor replaces that lower branch by L=3000Rv/(3000+Rv). A series ammeter burden Ra then gives total current 12/(2000+Ra+L) and indicated lower voltage IL. The ammeter current includes both lower-resistor and voltmeter currents; it does not equal the original lower-branch current by definition.

Check evidence and the limits of the model

Increasing input resistance reduces one loading effect, while reducing ammeter burden addresses another. Neither change removes source drift, resistor tolerance or calibration uncertainty. An exact correction based on assumed meter resistances is still conditional on those specifications. The diagram is a theoretical connectivity task only: no connection to a real battery, outlet, charged capacitor or unknown circuit is requested, and the numerical values are not equipment-selection guidance.

Worked original case

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.

Investigation

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.

Changed-case practice

Try the changed case before feedback

For the stated 2 kΩ/3 kΩ divider, let voltmeter resistance be 3 kΩ and ammeter burden zero. Find indicated lower voltage in V.

This practice is public and unsaved. A matching number does not verify understanding. Retain your explanation, assumptions and changed-case evidence in the separate course workspace.

Sources and evidence boundary

Original numerical cases and prose checked 30 October 2026 against the relevant primary explanation. All records are synthetic and all diagrams mathematical. No practical wiring, battery testing, capacitor handling, mains measurement or equipment safety rating is requested. Public feedback does not verify independent mastery; retain first predictions, contrasting recipes and criterion-based critique in the separate course evidence workspace.

Apply

The current measured upstream of both the lower resistor and voltmeter equals:

Public practice checks a specific claim. It does not establish independent mastery.

Which independent observation could reject this model rather than merely refit its parameters?

Continue

Completion requires a saved prediction, at least one capture and a reflection. Presence checks do not grade your reasoning.

Skipping retains experiments and awards no mastery.

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