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Electricity — charge, voltage and current

Distinguish electrical quantities and calculate current, power and transferred energy in an ideal resistor circuit.

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Prerequisites

Begin with charge

Electric charge can have positive or negative sign. Stationary charges of the same sign repel; opposite signs attract. A neutral object has zero net charge: its positive and negative charges balance.

For the arithmetic below, treat charge as an amount that can be counted across a chosen boundary. Keep the boundary and the time interval explicit.

Name the quantities

Current is charge flow per time. Voltage is electric potential difference: energy difference per unit charge. Resistance relates voltage and current for an ohmic element. Power is energy transferred per time.

Quantity Symbol used here Unit Useful relationship
Charge Q coulomb (C) 1 C = 1 A × 1 s
Current I ampere (A) I = charge / time, for a constant rate
Voltage V volt (V) 1 V = 1 J/C
Resistance R ohm (Ω) 1 Ω = 1 V/A
Power P watt (W) 1 W = 1 J/s

Do not confuse the symbol V for a voltage variable with V as its unit. Context distinguishes them. “3 V across the resistor” specifies a difference between its terminals, not a quantity of current stored inside it.

Solve an ideal circuit

Imagine an ideal 3 V source connected in a closed loop to one ideal 1000 Ω resistor. Ignore wire resistance and changes with temperature. For an ideal resistor, V = R × I. Rearranging gives I = V/R.

I = 3 V / 1000 Ω = 0.003 A = 3 mA
P = V × I = 3 V × 0.003 A = 0.009 W
energy in 2 s = 0.009 W × 2 s = 0.018 J
charge in 2 s = 0.003 A × 2 s = 0.006 C

The power expression follows by multiplying energy per charge by charge per time. The source supplies the energy that the resistor absorbs. Charge transport and energy transfer are related quantities, not interchangeable ones.

Change one assumption

Keep the voltage at 3 V and vary only the resistance in the same model:

Voltage (V) Resistance (Ω) Current (mA) Absorbed power (mW)
3 500 6 18
3 1000 3 9
3 2000 1.5 4.5

Doubling the resistance halves the current under a fixed voltage. That conclusion depends on both the ideal resistor law and the unchanged source voltage.

Try it yourself

For a 4 V source and ideal 2000 Ω resistor, calculate current, absorbed power and energy absorbed over 3 s. Then state which assumption lets you use V = R × I.

Answers and limits

The current is 2 mA, power is 8 mW and energy is 0.024 J. We assumed a constant ohmic resistance. The calculation uses ideal components. A real circuit also needs source limits and component ratings.

Next: fields and induction.

Verification record

  • Sources assessed by Codex (assistant)
  • Example checks recorded
  • Independent human review pending

Selected claims have been assessed against the passages below. This record does not certify every sentence or guarantee correctness.

Inspect claims, evidence and limitations

Source assessment: . 2 of 2 selected claims marked supported by the assessor. This is not a coverage percentage for the article.

  1. Electrical charge, potential difference, resistance and power have distinct SI units.

    Assessor finding: supported · definition · Article passage

    The selected statement is source-supported; numerical inputs and teaching scenarios in this article are original assumptions.

  2. The ideal resistor obeys V = R × I; the circuit abstraction replaces spatial fields with node voltages and branch currents.

    Assessor finding: supported · model · Article passage

    The selected statement is source-supported; numerical inputs and teaching scenarios in this article are original assumptions.

Reproducible checks

  • Recompute published resistor, force, flux, probability, level, thermal and lattice examples; check the reading prerequisite order.

    Passed on 2026-10-27

    node --test --test-name-pattern='physics examples respect circuit, field, quantum, energy and lattice models and reading prerequisites' src/library/physics.test.ts

Limits and open work

  • Introductory assistant assessment of selected claims; independent human review remains pending.
  • All numerical devices, amplitudes, levels and material parameters are stipulated examples, not measured properties or implementation specifications.

Independent human review

Pending. No independent human reviewer has signed off this version.

Content fingerprint: b8f598378a8eb13ca0b7572dd6e32ffa45e62ad26a3d5b431d2e6fc046172f3a. An article change invalidates this assessment.

Sources

  1. Steve Ward, Computation Structures — Circuits, sections 4.1–4.3
  2. NIST Guide to the SI — chapter 4, tables 3–4: electrical, energy and thermal units
  3. Feynman Lectures, volume II, chapter 1 — sections 1–1 and 1–2: forces and fields

Published by devutils · Updated · Original explanatory text; sources retain their own terms.