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 CThe 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.
Electrical charge, potential difference, resistance and power have distinct SI units.
Assessor finding: supported · definition · Article passage
- NIST Guide to the SI — chapter 4, tables 3–4: electrical, energy and thermal units — Chapter 4, tables 3–4, coulomb, volt, ohm, watt and joule rows
Passage read: Read the cited passage in the source page during preparation on 2026-10-25.
The selected statement is source-supported; numerical inputs and teaching scenarios in this article are original assumptions.
- NIST Guide to the SI — chapter 4, tables 3–4: electrical, energy and thermal units — Chapter 4, tables 3–4, coulomb, volt, ohm, watt and joule rows
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
- Steve Ward, Computation Structures — Circuits, sections 4.1–4.3 — Sections 4.2–4.3, lumped-element circuit and resistor constraint
Passage read: Read the cited passage in the source page during preparation on 2026-10-25.
The selected statement is source-supported; numerical inputs and teaching scenarios in this article are original assumptions.
- Steve Ward, Computation Structures — Circuits, sections 4.1–4.3 — Sections 4.2–4.3, lumped-element circuit and resistor constraint
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
- Steve Ward, Computation Structures — Circuits, sections 4.1–4.3
- NIST Guide to the SI — chapter 4, tables 3–4: electrical, energy and thermal units
- 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.