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Question: A piece of wire is cut into 5 equal parts. They are the connected parallel. If the equivalent resist...

A piece of wire is cut into 5 equal parts. They are the connected parallel. If the equivalent resistance of this combination is R{R}’, then the ratio RR\dfrac{R}{R'} is?

Explanation

Solution

Hint: Resistance is proportional to the length of wire and connecting nn resistors parallel reduces the resistance 1n\dfrac{1}{n} times.

Formula used: R=ρlAR = \dfrac{{\rho l}}{A} ; 1Reff=1R1+1R2+...+1Rn\dfrac{1}{{{R_{eff}}}} = \dfrac{1}{{{R_1}}} + \dfrac{1}{{{R_2}}} + ... + \dfrac{1}{{{R_n}}}

Complete step by step answer:
We know the resistance of a wire is proportional to the length of the wire (R=ρlA)\left( {\because R = \dfrac{{\rho l}}{A}} \right)
Let’s say the total resistance of the wire before cutting wasRR.
When we cut the wire into 5 parts, each one has a length of l5\dfrac{l}{5} and all other parameters remain unchanged.
So the resistance of each new segment isR5\dfrac{R}{5}.
Connecting them parallel gives a network as shown in fig1.

Now since the question asks for The effective resistance of this combination, lets recollect that the effective resistance of a parallel combination of nn resistances - R1{R_1},R2{R_2},R3{R_3}, . . . Rn{R_n} is given by: 1Reff=1R1+1R2+...+1Rn\dfrac{1}{{{R_{eff}}}} = \dfrac{1}{{{R_1}}} + \dfrac{1}{{{R_2}}} + ... + \dfrac{1}{{{R_n}}}
So if RR' is the resistance of this new combination, then:
1R=1R5+1R5+1R5+1R5+1R5\dfrac{1}{{R'}} = \dfrac{1}{{\dfrac{R}{5}}} + \dfrac{1}{{\dfrac{R}{5}}} + \dfrac{1}{{\dfrac{R}{5}}} + \dfrac{1}{{\dfrac{R}{5}}} + \dfrac{1}{{\dfrac{R}{5}}}
Simplifying this expression a bit gives us:
1R=5R5\dfrac{1}{{R'}} = \dfrac{5}{{\dfrac{R}{5}}}
R=R25R' = \dfrac{R}{{25}}
So the ratio RR=25\dfrac{R}{R'}=25 , which is the required answer.

Additional Information:
Here the wire was cut and hence the area remained constant. In cases where wire is stretched to a new length, resistance is not proportional to length.
In cases of stretching, since its volume VV that is conserved, The Resistance RR can be related with length ll as R=ρlA=ρl×lA×l=ρl2VR = \dfrac{{\rho l}}{A} = \dfrac{{\rho l \times l}}{{A \times l}} = \dfrac{{\rho {l^2}}}{V}.
Thus in case of stretching, the resistance varies as Rl2R \propto {l^2}

Note: We can answer this question quicker by remembering some special cases in parallel. When we have nn equal resistances each of resistance RR connected parallel, the effective resistance becomes Rn\dfrac{R}{n}.
Here since we have 5 resistances, each of Resistance R5\dfrac{R}{5}
R=R55=R25R' = \dfrac{{\dfrac{R}{5}}}{5} = \dfrac{R}{{25}}
So RR=25\dfrac{R}{{R'}} = 25