Physic Labs

Electricity and magnetism

Electric current

Observe DC current through a model of drifting electrons in a wire. Verify I=ΔQ/ΔtI = \Delta Q/\Delta t and the roles of cross-section and carrier density in I=neAvdI = neAv_d.

Middle school

⚠ Virtual simulation; when measuring real current, connect the ammeter in series and never across a voltage source — short-circuit hazard.

Equipment

  • Virtual metal wire with moving free-electron dots
  • Current slider (1–8)
  • Sliders for relative cross-section and carrier density
  • Time slider and a charge counter

Procedure

  1. Track electron drift and conventional current

    Run the simulation: blue dots (electrons) drift one way while the red arrow — conventional current — points opposite. Electrons show random thermal motion plus a small drift; conventional current runs from the positive to the negative terminal.

  2. Count charge versus time

    Set a current value and drag the time slider: accumulated charge grows proportionally, Q=ItQ = It. Read the counter at two instants and check that I=ΔQ/ΔtI = \Delta Q/\Delta t stays constant for steady current.

  3. Vary cross-section and carrier density

    Hold I fixed and increase cross-section A: for the same current, the drift speed must fall per vd=I/(neA)v_d = I/(neA). Vary density n similarly. Predict first whether electrons drift faster or slower in a thinner wire, then observe.

Simulation

Experiment history

In 1800 Alessandro Volta built the voltaic pile, giving a continuous current for the first time. André-Marie Ampère built electrodynamics in 1820–1826, defining conventional current direction and measuring interactions between current-carrying wires — the ampere is named for him. In 1876–1883 Edwin Hall's Hall-effect measurements showed charge carriers in metals are negative; J.J. Thomson's discovery of the electron in 1897 identified the actual carrier. Paul Drude in 1900 modeled conduction with the drift picture I=neAvdI = neAv_d.

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