Question #154339

By considering the principles that the distribution of current in a circuit is the result of charge conservation, and the distribution of potential differences in a circuit is the result of energy conservation, derive:

(a) the combined resistance of two resistors R1 and R2 connected in series (4 marks)

(b) the combined resistance of two resistors R1 and R2 connected in parallel.


1
Expert's answer
2021-01-10T18:28:43-0500

Explanations & Calculations



a)

  • In the first circuit, potential difference (V) is distributed among the resistors while the same current flows through both of them (energy conserved: V= energy per unit charge)
  • Therefore,

V=VR1+VR2=i1R1+i1R2=i(R1+R2)\qquad\qquad \begin{aligned} \small V&= \small V_{R_1}+V_{R_2}\\ &= \small i_1R_1+i_1R_2\\ &= \small i(R_1+R_2) \end{aligned}

  • When the equivalent resistance is considered the same current should be flowing through it therefore,

V=iReq\qquad\qquad \begin{aligned} \small V&= \small iR_{eq} \end{aligned}

  • Equalling both the equations yield,

iReq=i((R1+R2)Req=R1+R2\qquad\qquad \begin{aligned} \small iR_{eq}&= \small i((R_1+R_2)\\ \small R_{eq}&= \small R_1+R_2 \end{aligned}


b)

  • In a parallel connection, the same potential difference is sensed by both the resistors while the current is additive (charge conservation).
  • Therefore,

itotal=i1+i2=VR1+VR2\qquad\qquad \begin{aligned} \small i_{total}&= \small i_1+i_2\\ &= \small \frac{V}{R_1}+\frac{V}{R_2}\\ \end{aligned}

  • When the equivalent resistance is considered for this circuit, the same total current should flow through it under the same potential difference.
  • Therefore,

itotal=VReq\qquad\qquad \begin{aligned} \small i_{total}&= \small \frac{V}{R_{eq}}\\ \end{aligned}

  • As the 2 equations are combined it gives,

VReq=VR1+VR21Req=1R1+1R2Req=R1R2R1+R2\qquad\qquad \begin{aligned} \small \frac{V}{R_{eq}}&= \small \frac{V}{R_1}+\frac{V}{R_2}\\ \small \frac{1}{R_{eq}}&= \small \frac{1}{R_1}+\frac{1}{R_2}\\ \small R_{eq}&= \small \frac{R_1R_2}{R_1+R_2} \end{aligned}





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