Explain current without consuming charge
Current is the rate at which charge crosses a chosen section: I=ΔQ/Δt, measured in amperes, or coulombs per second. It has a direction convention but is not a spatial vector added by geometric components. Conventional current follows the direction positive charge would move. In a metal the mobile electrons drift in the opposite direction.
Learning outcome: Capture current 0.20 A at areas 0.5, 1.0 and 2.0 mm². Reconcile the identical charge-time slope with changing drift speed. Then increase current alone and explain which graph feature changes.
Starting recap
Distinguish charge flow from energy transfer. Identify nodes, choose consistent current/voltage signs and state source and initial conditions before applying algebra.
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Try
At 0.20 A, 2.0 C passes a section in 10 s, corresponding to about 1.248×10¹⁹ electrons in magnitude. For n=8×10²⁸ m⁻³ and A=1 mm², the supplied formula gives vd≈0.01560 mm/s. The downstream steady current is still 0.20 A.
Open the experimentPredict
At fixed current, will doubling the area double the transported charge in 10 s, or change the drift speed instead?
Experiment
Capture current 0.20 A at areas 0.5, 1.0 and 2.0 mm². Reconcile the identical charge-time slope with changing drift speed. Then increase current alone and explain which graph feature changes.
Track transported charge and drift without consuming current
Worked teaching model · synthetic values · Uniform hypothetical metallic wire: carrier density 8×10²⁸ m⁻³, electron charge magnitude 1.602176634×10⁻¹⁹ C. Steady current, no accumulation. Electron drift opposes conventional current. Drift calculation is supplied microscopic enrichment, not a signal-propagation speed.
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Circuit connections: Closed path with one wire section before and another after a resistive element; both carry the same steady current.
Axes rescale with settings; compare numerical values, not screen angles or apparent lengths. Solid/points show the selected model relationship or observations; the dashed comparison is explained below.
| Quantity | Value | Unit |
|---|---|---|
| Charge passing in 10 s | 2 | C |
| Electron count passing in 10 s | 12483000000000000000 | electrons |
| Electron drift speed magnitude | 0.015604 | mm/s |
| Current at downstream section | 0.2 | A |
Accessible plot coordinates
| elapsed time (s) | transported conventional charge (C) |
|---|---|
| 0 | 0 |
| 1 | 0.2 |
| 2 | 0.4 |
| 3 | 0.6 |
| 4 | 0.8 |
| 5 | 1 |
| 6 | 1.2 |
| 7 | 1.4 |
| 8 | 1.6 |
| 9 | 1.8 |
| 10 | 2 |
The charge–time slope is current; charges transfer energy without being consumed.
Carrier random thermal motion does not imply net current. Electron drift is opposite the chosen conventional current and is not the speed at which an electrical disturbance propagates. Doubling area at fixed current halves drift speed.
The charge–time slope is current; charges transfer energy without being consumed.
Carrier random thermal motion does not imply net current. Electron drift is opposite the chosen conventional current and is not the speed at which an electrical disturbance propagates. Doubling area at fixed current halves drift speed.
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Explain why a battery supplies energy rather than a one-way stock of electrons that disappears in a resistor.
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