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Resistances in Parallel

Same voltage across each resistor; currents add. For two resistors: R_eq = R₁R₂/(R₁+R₂). R_eq is always less than the smallest individual resistance.
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Derivation

Derivation

In parallel, the same voltage VV appears across each resistor. Individual currents:

I1=VR1,I2=VR2,,In=VRnI_1 = \frac{V}{R_1},\quad I_2 = \frac{V}{R_2},\quad \ldots,\quad I_n = \frac{V}{R_n}

Total current (KCL at junction):

I=I1+I2++In=V(1R1+1R2++1Rn)I = I_1 + I_2 + \cdots + I_n = V\left(\frac{1}{R_1} + \frac{1}{R_2} + \cdots + \frac{1}{R_n}\right) 1Req=1R1+1R2++1Rn\boxed{\frac{1}{R_{eq}} = \frac{1}{R_1} + \frac{1}{R_2} + \cdots + \frac{1}{R_n}}

Two-resistor formula

Req=R1R2R1+R2R_{eq} = \frac{R_1 R_2}{R_1 + R_2}

Key property

Req<RminR_{eq} < R_{min} — always less than the smallest resistor. Parallel connection is like increasing the cross-sectional area of a conductor.

Current divider

For two parallel resistors, current splits inversely with resistance:

I1I2=R2R1\frac{I_1}{I_2} = \frac{R_2}{R_1}

The smaller resistor carries the larger current.