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Resistors in Circuits

The total resistance of resistors in parallel is always less than the smallest resistor in the parallel network.

Resistors in parallel

Resistors in parallel

  • The reciprocal total resistance, 1Rtotal\frac{1}{R_{total}}, is the sum of the reciprocal resistances in the network.
  • It can be written for a network of n resistors as:
    • 1RTOTAL=1R1+1R2++1Rn\frac{1}{R_{TOTAL}}= \frac{1}{R_1}+\frac{1}{R_2}+⋯+\frac{1}{R_n}
Resistors in series

Resistors in series

  • The total resistance is the sum of each individual resistor.
  • The equation for the total resistance is:
    • Rtotal=R1+R2+...+Rn{R_{total}}={R_1}+{R_2}+...+{R_n}
      • Where n is the number of resistors.

Current in Parallel Circuits

Current in parallel circuits splits up like a river's current.

Kirchhoff's first law

Kirchhoff's first law

  • The total current arriving at a junction is equal to the total current leaving a junction.
  • The current labelled is conventional current (positive to negative).
  • For electrical parallel circuits, this results in the familiar "current splits up" rule.
  • This is a demonstration of the conservation of charge. Charge cannot be created or destroyed.

Voltage in Parallel Circuits

The sum of voltage drops in a closed loop must be equal to zero.

Kirchhoff's second law

Kirchhoff's second law

  • The sum of voltage drops in a closed loop must be equal to zero.
Kirchhoff's second law 2

Kirchhoff's second law 2

  • This also applies to having identical cells in parallel.
  • The voltage drop across a reversed cell is negative because a positive charge does work against the positive end of the cell.
Kirchhoff's second law 3

Kirchhoff's second law 3

  • This is a demonstration of the conservation of energy.
  • If the sum of voltage drops was not zero, there would be either the destruction or creation of energy - which is impossible.
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