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Resistor

A resistor is a passive linear dipole such that the voltage across its terminals is proportional to the current passing through it.

Resistor IEC

IEC symbol

or

Resistor IEEE

IEEE symbol

Inductance

The resistance unit is the Ohm (Ω\Omega). It can also be defined with Siemens (SS) as the reciprocal of the resistance.

Ω=1S\Omega = \frac{1}{S} U=RIU = R \cdot I

where:

  • UU: voltage in Volts (V)
  • II: current in Amperes (A)
  • RR: resistance in Ohms (Ω\Omega)

Or using the conductance:

I=GUI = G \cdot U

where:

  • G=1RG = \frac{1}{R} is the conductance in Siemens (S)

The resistance of a wire-like conductor with a uniform cross-section is given by:

R=ρlAR = \rho \cdot \frac{l}{A}

where:

  • ρ\rho: resistivity of the material (Ω.m\Omega.m)
  • ll: length of the wire (m)
  • AA: cross-sectional area of the wire (m²)
Resistors in Series

A circuit composed of multiple resistors connected in series can be reduced to a single equivalent resistance ReR_e, given by:

Re=R1+R2++RnR_e = R_1 + R_2 + \dots + R_n
Resistors in Series
Resistors in Parallel

A circuit composed of multiple resistors connected in parallel can be reduced to a single equivalent resistance ReR_e, given by:

1Re=1R1+1R2++1Rn\frac{1}{R_e} = \frac{1}{R_1} + \frac{1}{R_2} + \dots + \frac{1}{R_n}
Resistors in Parallel

For two resistors:

1Re=1R1+1R2\frac{1}{R_e} = \frac{1}{R_1} + \frac{1}{R_2}

The formula can be simplified to:

Re=R1R2R1+R2R_e = \frac{R_1 * R_2}{R_1 + R_2}
Details1Re=1R1+1R2\frac{1}{R_e} = \frac{1}{R_1} + \frac{1}{R_2} 1Re(R1R2)=(1R1+1R2)(R1R2)\frac{1}{R_e} * (R_1 * R_2) = (\frac{1}{R_1} + \frac{1}{R_2}) * (R_1 * R_2) R1R2Re=R1R2R1+R1R2R2\frac{R_1 * R_2}{R_e} = \frac{R_1 * R_2}{R_1} + \frac{R_1 * R_2}{R_2} R1R2Re=R2+R1\frac{R_1 * R_2}{R_e} = R_2 + R_1 1Re=R2+R1R1R2\frac{1}{R_e} = \frac{R_2 + R_1}{R_1 * R_2} Re=R1R2R2+R1=R1R2R1+R2R_e = \frac{R_1 * R_2}{R_2 + R_1} = \frac{R_1 * R_2}{R_1 + R_2}