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Question: A copper wire of length \(l\) and radius \(r\) is nickel plated till its final radius is \(R\) and l...

A copper wire of length ll and radius rr is nickel plated till its final radius is RR and length ll . If the specific resistance of nickel and copper be ρn{\rho _n} and ρc{\rho _c}, then the conductance of wire with nickel plating is:
A) πr2lρc\dfrac{{\pi {r^2}}}{{l{\rho _c}}}
B) π(R2r2)lρn\dfrac{{\pi ({R^2} - {r^2})}}{{l{\rho _n}}}
C) πl[r2ρc+R2r2ρn]\dfrac{\pi }{l}\left[ {\dfrac{{{r^2}}}{{{\rho _c}}} + \dfrac{{{R^2} - {r^2}}}{{{\rho _n}}}} \right]
D) lρcπr2+lρnπ(R2r2)\dfrac{{l{\rho _c}}}{{\pi {r^2}}} + \dfrac{{l{\rho _n}}}{{\pi \left( {{R^2} - {r^2}} \right)}}

Explanation

Solution

In this problem, we can treat the whole wire as a copper wire and having nickel wire (plating) connected in parallel. Calculate the conductance of copper wire and nickel wire separately. The effective conductance will be the same as the sum of two conductances connected in parallel.

Complete step by step solution:
In this problem, as we have discussed in the hint above, the copper wire after nickel plating will act as two conductances in parallel. Let us find the conductance for the copper wire.
As per the given information,
ll is the length of the copper wire
rr is the initial radius of the copper wire
ρc{\rho _c} is the specific resistance of the copper wire
The conductance of copper wire Gc{G_c} will be given as
Gc=arealength×specificresistance{G_c} = \dfrac{{area}}{{length \times specific\,resistance}}
The copper wire is circular in shape, the area of the copper wire will be given as
area=πr2area = \pi {r^2}
Thus, the conductance of the copper wire will be
Gc=πr2l×ρc{G_c} = \dfrac{{\pi {r^2}}}{{l \times {\rho _c}}}--equation 11
After the nickel plating is done, the new dimensions will be
ll is the length of the nickel plating
RrR - r is the radius of the nickel plating
ρn{\rho _n} is the specific resistance of nickel
The conductance of nickel wire Gn{G_n} will be given as
Gn=arealength×specificresistance{G_n} = \dfrac{{area}}{{length \times specific\,resistance}}
The nickel-plated wire will be circular in shape, the area of this nickel wire will be given as
area=π(R2r2)area = \pi ({R^2} - {r^2})
Thus, the conductance of the nickel wire will be
Gn=π(R2r2)l×ρn{G_n} = \dfrac{{\pi \left( {{R^2} - {r^2}} \right)}}{{l \times {\rho _n}}}--equation 22
The effective conductance of two systems in parallel is the arithmetic sum of their individual conductance. Therefore, the effective conductance Geffective{G_{effective}} will be given as
Geffective=Gc+Gn{G_{effective}} = {G_c} + {G_n}
Substituting the value from equation 11 and equation 22 , we can have
Geffective=πr2l×ρc+π(R2r2)l×ρn{G_{effective}} = \dfrac{{\pi {r^2}}}{{l \times {\rho _c}}} + \dfrac{{\pi \left( {{R^2} - {r^2}} \right)}}{{l \times {\rho _n}}}
Taking πl\dfrac{\pi }{l} common, we can have
Geffective=πl[r2ρc+(R2r2)ρn]{G_{effective}} = \dfrac{\pi }{l}\left[ {\dfrac{{{r^2}}}{{{\rho _c}}} + \dfrac{{\left( {{R^2} - {r^2}} \right)}}{{{\rho _n}}}} \right]
Thus, the conductance of wire with nickel plating is πl[r2ρc+(R2r2)ρn]\dfrac{\pi }{l}\left[ {\dfrac{{{r^2}}}{{{\rho _c}}} + \dfrac{{\left( {{R^2} - {r^2}} \right)}}{{{\rho _n}}}} \right] siemens.

Therefore, option C is the correct option.

Note: Conductance is the inverse of resistance. Similarly, conductivity is the inverse of resistivity. Remember that the effective conductance for two conductors is the arithmetic sum of their individual conductance. The SI unit of electrical conductance is siemens, it is inverse of ohm.