One route or two?
In series, every charge path passes through both loads, so the same current flows through them. In parallel, the path branches. Each branch sees the source voltage, and the source supplies the sum of the branch currents.
Close a switch. Follow a complete path. Give current a second route and discover what changes.
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Electric current is the rate at which charge passes a point. A source transfers energy to the circuit; a lamp transfers energy to light and heat. Charge keeps circulating—it is not used up by the lamp.
Two equal loads are in series. Is there less current after the first one?
Both are on the same unbranched path. The loads transfer energy, while the current remains the same. Switch to parallel and compare branch currents instead.
In series, every charge path passes through both loads, so the same current flows through them. In parallel, the path branches. Each branch sees the source voltage, and the source supplies the sum of the branch currents.
The cell, contacts, switch and light source form a circuit. Our cutaway follows an older incandescent flashlight with a return conductor through its body. The constant-resistance lamp is an idealization; modern LED flashlights use a different load and often a driver circuit.
Voltage is energy transferred per unit charge. Across a resistor, electrical energy becomes thermal energy. The moving marks indicate conventional current from positive to negative outside the battery; electrons in metal drift the other way.
For these ideal fixed resistors, I = V/R. Series: Rₑ = R₁ + R₂. Parallel: 1/Rₑ = 1/R₁ + 1/R₂. An open switch gives I = 0. We omit switching transients and use the settled DC state.
P = VI = I²R. In series, V₁ + V₂ = Vsource. At a parallel junction, I₁ + I₂ = Isource. Adding the load powers gives the source power. That is an energy balance, not a calibrated brightness scale.
A filament heats up and changes resistance, so doubling voltage need not double its current. The battery also has internal resistance. The virtual source stays at its selected voltage; the glow shows relative modeled power, not lumens or temperature.
Keep the flashlight assembled. Sketch a loop containing a battery, switch and light source. Predict where the loop is interrupted when the switch is off.
Point the light at the paper, away from eyes. Turn the normal switch on and off. Compare the result with the open and closed switch here.
Read any visible LED or bulb label without dismantling the light. Record which parts the outside view hides. An LED lamp needs a different electrical model from our ideal resistor.
Which part opens the path when you turn the light off?
Use only the flashlight’s normal controls and manufacturer instructions. No disassembly or new wiring. This observation cannot measure current, resistance or the speed of electricity.
University Physics Volume 2 §9.1, Eqs. 9.1–9.3 and direction-of-current discussion. Supports the current definition and marker convention.
OpenStax · Electric currentUniversity Physics Volume 2 §10.2, Eqs. 10.2–10.3 and junction/loop derivation. Supports solver and two-load schematics.
OpenStax · Series & parallelUniversity Physics Volume 2 §9.6. P = VI and resistor-power relationships support numerical outputs, not the brightness rendering.
OpenStax · Electrical powerUniversity Physics Volume 2 §9.3, resistivity versus temperature; scopes the fixed-resistance filament analogy.
OpenStax · ResistanceIndependent subject review is pending.
Read the sources and model assumptions