
A wire of radius r has resistance R. If it is stretched to a radius of \[\dfrac{{3r}}{4}\] its resistance becomes.
A. \[\dfrac{{9R}}{{16}} \\ \]
B. \[\dfrac{{16R}}{9} \\ \]
C. \[\dfrac{{81R}}{{256}} \\ \]
D. \[\dfrac{{256R}}{{81}}\]
Answer
162.9k+ views
Hint:When the wire is stretched then the volume of the material of which the wire is made of remains constant as well as the resistivity of the material of the wire.
Formula used:
\[R = \dfrac{{\rho l}}{A}\]
where R is the resistance of the wire of length l and cross-sectional area A, \[\rho \] is the resistivity of the material of the wire.
Complete step by step solution:
Resistance of wire is given as \[R = \dfrac{{\rho l}}{A}\]
The volume of the wire is the product of the length and the cross-section.
Also volume of wire having length l and the area of cross-section A will be,
\[V = Al\]
If the final length is \[{l_f}\] and cross-section is \[{A_f}\] then the final volume will be equal to the initial volume of the wire,
\[{V_i} = {V_f}\]
\[\Rightarrow {A_i}{l_i} = {A_f}{l_f}\]
\[\Rightarrow \dfrac{{{l_i}}}{{{l_f}}} = \dfrac{{{A_f}}}{{{A_i}}}\]
Initially the radius of the wire is r.
Now the wire is stretched then the radius of the wire is \[\dfrac{{3r}}{4}\].
\[\dfrac{{{A_i}}}{{{A_f}}} = \dfrac{{\pi r_i^2}}{{\pi r_f^2}}\]
\[\Rightarrow \dfrac{{{A_i}}}{{{A_f}}} = \dfrac{{{r^2}}}{{{{\left( {\dfrac{{3r}}{4}} \right)}^2}}}\]
\[\Rightarrow \dfrac{{{A_i}}}{{{A_f}}} = \dfrac{{16}}{9}\]
So, the ratio of the final length to the initial length of the wire is,
\[\dfrac{{{l_f}}}{{{l_i}}} = \dfrac{{{A_i}}}{{{A_f}}} = \dfrac{{16}}{9}\]
The initial resistance of the wire is,
\[{R_i} = \dfrac{{\rho {l_i}}}{{{A_i}}}\]
The final resistance of the wire is,
\[{R_f} = \dfrac{{\rho {l_f}}}{{{A_f}}}\]
The initial resistance of the wire is given as R. We need to find the final resistance of the wire.
Taking the ratio of the initial resistance of the wire to the final resistance, we get
\[\dfrac{{{R_i}}}{{{R_f}}} = \dfrac{{\dfrac{{\rho {l_i}}}{{{A_i}}}}}{{\dfrac{{\rho {l_f}}}{{{A_f}}}}} \\ \]
\[\Rightarrow \dfrac{R}{{{R_f}}} = \left( {\dfrac{{{A_f}}}{{{A_i}}}} \right) \times \left( {\dfrac{{{l_i}}}{{{l_f}}}} \right) \\ \]
\[\Rightarrow \dfrac{R}{{{R_f}}} = \left( {\dfrac{9}{{16}}} \right) \times \left( {\dfrac{9}{{16}}} \right) \\ \]
\[\Rightarrow \dfrac{R}{{{R_f}}} = \dfrac{{81}}{{256}} \\ \]
\[\therefore {R_f} = \dfrac{{256R}}{{81}}\]
Hence, the final resistance of the wire is \[\dfrac{{256R}}{{81}}\].
Therefore, the correct option is D.
Note: The material characteristic is resistivity. No matter how large or small, a resistor constructed of the same material will have the same resistivity. Unlike resistivity, which does not depend on the conductor's length or cross-sectional area, resistance does.
Formula used:
\[R = \dfrac{{\rho l}}{A}\]
where R is the resistance of the wire of length l and cross-sectional area A, \[\rho \] is the resistivity of the material of the wire.
Complete step by step solution:
Resistance of wire is given as \[R = \dfrac{{\rho l}}{A}\]
The volume of the wire is the product of the length and the cross-section.
Also volume of wire having length l and the area of cross-section A will be,
\[V = Al\]
If the final length is \[{l_f}\] and cross-section is \[{A_f}\] then the final volume will be equal to the initial volume of the wire,
\[{V_i} = {V_f}\]
\[\Rightarrow {A_i}{l_i} = {A_f}{l_f}\]
\[\Rightarrow \dfrac{{{l_i}}}{{{l_f}}} = \dfrac{{{A_f}}}{{{A_i}}}\]
Initially the radius of the wire is r.
Now the wire is stretched then the radius of the wire is \[\dfrac{{3r}}{4}\].
\[\dfrac{{{A_i}}}{{{A_f}}} = \dfrac{{\pi r_i^2}}{{\pi r_f^2}}\]
\[\Rightarrow \dfrac{{{A_i}}}{{{A_f}}} = \dfrac{{{r^2}}}{{{{\left( {\dfrac{{3r}}{4}} \right)}^2}}}\]
\[\Rightarrow \dfrac{{{A_i}}}{{{A_f}}} = \dfrac{{16}}{9}\]
So, the ratio of the final length to the initial length of the wire is,
\[\dfrac{{{l_f}}}{{{l_i}}} = \dfrac{{{A_i}}}{{{A_f}}} = \dfrac{{16}}{9}\]
The initial resistance of the wire is,
\[{R_i} = \dfrac{{\rho {l_i}}}{{{A_i}}}\]
The final resistance of the wire is,
\[{R_f} = \dfrac{{\rho {l_f}}}{{{A_f}}}\]
The initial resistance of the wire is given as R. We need to find the final resistance of the wire.
Taking the ratio of the initial resistance of the wire to the final resistance, we get
\[\dfrac{{{R_i}}}{{{R_f}}} = \dfrac{{\dfrac{{\rho {l_i}}}{{{A_i}}}}}{{\dfrac{{\rho {l_f}}}{{{A_f}}}}} \\ \]
\[\Rightarrow \dfrac{R}{{{R_f}}} = \left( {\dfrac{{{A_f}}}{{{A_i}}}} \right) \times \left( {\dfrac{{{l_i}}}{{{l_f}}}} \right) \\ \]
\[\Rightarrow \dfrac{R}{{{R_f}}} = \left( {\dfrac{9}{{16}}} \right) \times \left( {\dfrac{9}{{16}}} \right) \\ \]
\[\Rightarrow \dfrac{R}{{{R_f}}} = \dfrac{{81}}{{256}} \\ \]
\[\therefore {R_f} = \dfrac{{256R}}{{81}}\]
Hence, the final resistance of the wire is \[\dfrac{{256R}}{{81}}\].
Therefore, the correct option is D.
Note: The material characteristic is resistivity. No matter how large or small, a resistor constructed of the same material will have the same resistivity. Unlike resistivity, which does not depend on the conductor's length or cross-sectional area, resistance does.
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