Prerequisites
Describe a field
A field assigns a physical quantity to positions in space and, when needed, time. Electric and magnetic fields have magnitude and direction. For a stationary test charge q, the electric force is q × E. For a moving charge, the full law also includes a magnetic contribution.
A vector is a quantity with direction as well as magnitude. Here we start with one line: choose right as the positive direction and left as negative. This keeps the arithmetic simple without pretending that real fields have only one dimension.
Follow the sign of a force
In an invented uniform electric field of +200 N/C, place a small positive test charge of +0.000002 C. Assume it does not disturb the source of the field.
force = charge × electric field
force = 0.000002 C × 200 N/C = +0.0004 NIts force points right. Replacing it with a charge of the same magnitude and opposite sign reverses that force. A force specifies a push, not the object's current velocity; determining motion would also require its mass and initial conditions.
| Test charge (μC) | Electric field (N/C) | Electric force (μN) |
|---|---|---|
| 2 | 200 | 400 |
| -2 | 200 | -400 |
| 1 | 200 | 200 |
These values describe a prescribed field, not a method for constructing it.
Let a changing flux produce a voltage
Magnetic flux summarizes the magnetic field passing through an oriented surface. In a simple fixed loop, a changing flux produces an electromotive force, or emf, measured in volts. The induction reference gives the negative flux-change rate; the minus sign depends on the agreed loop and surface orientations.
For a fictional single-turn fixed loop, assume the signed flux increases uniformly from 0.001 Wb to 0.004 Wb in 0.003 s. Wb means weber, a unit equal to V × s.
flux change = 0.004 Wb - 0.001 Wb = 0.003 Wb
emf = -0.003 Wb / 0.003 s = -1 VThis calculation predicts an emf. It does not specify a current: that also depends on the connected circuit. A constant flux through this fixed loop gives zero induced emf from this mechanism.
Try it yourself
- What is the electric force on +1 μC in a field of -300 N/C?
- If a fixed loop's signed flux increases by 0.006 Wb in 0.003 s, what emf follows under the same orientation convention?
- Does the emf alone determine the current?
Answers and limits
The force is -300 μN. The emf is -2 V. Current still requires a circuit model. These idealized exercises omit field geometry calculations, self-inductance and radiation; they do not describe a practical coil or transformer design.
Next: quantum basics.
Verification record
- Sources assessed by Codex (assistant)
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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.
An electric field assigns a vector to each position and time; the electric force on a stationary charge is q × E.
Assessor finding: supported · definition · Article passage
- Feynman Lectures, volume II, chapter 1 — sections 1–1 and 1–2: forces and fields — Sections 1–1 and 1–2, equation 1.1 and definition of a field
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.
- Feynman Lectures, volume II, chapter 1 — sections 1–1 and 1–2: forces and fields — Sections 1–1 and 1–2, equation 1.1 and definition of a field
Changing magnetic flux induces an emf; for a fixed loop the circulation of the electric field is minus the flux change rate.
Assessor finding: supported · model · Article passage
- Feynman Lectures, volume II, chapter 17 — section 17–1: induction — Section 17–1, equations 17.1–17.3 and the fixed-circuit flux rule
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.
- Feynman Lectures, volume II, chapter 17 — section 17–1: induction — Section 17–1, equations 17.1–17.3 and the fixed-circuit flux rule
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: 6226fe590770ef073c7ff40012d55850d29126fb56e3d8740bd1fa7e28405d7e. An article change invalidates this assessment.
Sources
- Feynman Lectures, volume II, chapter 1 — sections 1–1 and 1–2: forces and fields
- Feynman Lectures, volume II, chapter 17 — section 17–1: induction
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