Circuit diagram: 2 Marks
Derivation: 3 Marks
In the parallel combination of resistors, one end of each resistor is connected at one point (say A) and the other end of each resistor is connected at the other point (Say B).
A cell is then connected in between these points A and B through a key as shown in Fig. 8.26.
Let R be the equivalent resistance, V be the potential difference applied between the ends A and B and I be the current that enters at A. Then the current I divides itself into three branches
I1,I2 and I3 flowing through the resistors
R1,R2 and R3 respectively.
Total current,
I=I1+I2+I3 ...(i)
Potential difference between A and B,
V=I1R1=I2R2=I3R3 Or
I1=VR1 ,
I2=VR2 ,and
I3=VR3 As R is the equivalent resistance and I the total current,
∴I=VR Substituting
I=VR in Eq. (i), we get :
VR=VR1+VR2+VR3 Or
1R=1R1+1R2+1R3 Thus, when three or more resistors are connected in parallel, the reciprocal of the combined resistance is equal to the sum of the reciprocal of the individual resistances.