
An aluminium (${\alpha _{Al}} = 4 \times {10^{ - 3}}\;{\rm{l}}^\circ {\rm{C}}$) wire resistance ‘${R_1}$’ and carbon wire (${\alpha _C} = 0.5 \times {10^{ - 3}}\;{\rm{l}}^\circ {\rm{C}}$) resistance ‘${R_2}$’ are connected in series to have a resultant resistance of $18\;{\rm{ohm}}$ at all temperatures. The values of ${R_1}$ and ${R_1}$ in ohms
A.$2$, $16$
B. $12$, $6$
C. $13$, $5$
D. $14$, $4$
Answer
566.4k+ views
Hint:In this question, we can use the theory that the resistance of a combination of wires is independent of the variation in temperature. Using the expression for the resultant resistance of the wires in series and the expression for the resultant resistance after a variation in temperature we can find the solution.
Complete step by step answer:
Given:
The temperature coefficient of resistance of aluminium, ${\alpha _{Al}} = 4 \times {10^{ - 3}}\;{\rm{l}}^\circ {\rm{C}}$
The temperature coefficient of resistance of carbon, ${\alpha _C} = 0.5 \times {10^{ - 3}}\;{\rm{l}}^\circ {\rm{C}}$
The resistance of aluminium wire is${R_1}$ .
The resistance of carbon wire is ${R_2}$ .
When wires of resistances ${R_1}$ and ${R_2}$ are connected in series, we can write the resultant resistance of the wires as
$R = {R_1} + {R_2}$
Here $R$ is the resultant resistance of wires of resistances ${R_1}$ and${R_2}$.
We can substitute $18\;\Omega $ for $R$ in in the above equation, we get
${R_1} + {R_2} = 18\;\Omega $
Let the temperature of the wires are increased by $\Delta T$. Then
The new resistance of the aluminium wire, ${{R_1}^1} = {R_1}\left( {1 + {\alpha _{Al}}\Delta T} \right)$
The new resistance of the carbon wire, ${{R_2}^1} = {R_2}\left( {1 + {\alpha _C}\Delta T} \right)$
When wires of resistances ${{R_1}^1}$ and ${{R_2}^1}$ are connected in series, we can write the resultant resistance of the wires as
${R^1} = {{R_1}^1} + {{R_2}^1}$
Here ${R^1}$ is the resultant resistance of ${{R_1}^1}$ and ${{R_2}^1}$ connected in series.
The resistances of a combination of wires remain the same even if the temperatures of the wires are increased. Hence, we can equate the resistances $R$ and ${R^1}$ to get
$
R = {R^1}\\
{R_1} + {R_2} = {{R_1}^1} + {{R_2}^1}
$
Substituting ${R_1}\left( {1 + {\alpha _{Al}}\Delta T} \right)$ for ${{R_1}^1}$ and ${R_2}\left( {1 + {\alpha _C}\Delta T} \right)$ for${{R_2}^1}$, we get
$
{R_1} + {R_2} = {R_1}\left( {1 + {\alpha _{Al}}\Delta T} \right) + {R_2}\left( {1 + {\alpha _C}\Delta T} \right)\\
\Rightarrow{R_1} + {R_2} = {R_1} + {R_1}{\alpha _{Al}}\Delta T + {R_2} + {R_2}{\alpha _C}\Delta T\\
\Rightarrow{R_2}{\alpha _C}\Delta T = - {R_1}{\alpha _{Al}}\Delta T
$
We can avoid the negative sign in the equation.
So, rewriting the above equation, we get
$\dfrac{{{R_2}}}{{{R_1}}} = \dfrac{{{\alpha _{Al}}}}{{{\alpha _C}}}$
Hence, we obtained an equation in the form of the ratio between ${R_2}$ and${R_1}$ .
Substituting $4 \times {10^{ - 3}}\;{\rm{l}}^\circ {\rm{C}}$ for ${\alpha _{Al}}$ and $0.5 \times {10^{ - 3}}\;{\rm{l}}^\circ {\rm{C}}$ for ${\alpha _C}$ in the above equation, we get
$
\dfrac{{{R_2}}}{{{R_1}}} = \dfrac{{4 \times {{10}^{ - 3}}\;{\rm{l}}^\circ {\rm{C}}}}{{0.5 \times {{10}^{ - 3}}\;{\rm{l}}^\circ {\rm{C}}}}\\
\Rightarrow\dfrac{{{R_2}}}{{{R_1}}} = 8\\
\Rightarrow{R_2} = 8{R_1}
$
Substituting $8{R_1}$ for ${R_2}$ in ${R_1} + {R_2} = 18\;\Omega $, we get
$
{R_1} + 8{R_1} = 18\;\Omega \\
\Rightarrow 9{R_1} = 18\;\Omega \\
\Rightarrow{R_1} = 2\;\Omega
$
Hence, we obtained the value of the resistance of the aluminium wire as$2\;\Omega $.
Substituting $2\;\Omega $ for ${R_1}$ in the equation${R_1} + {R_2} = 18\;\Omega $, we obtain
$
{R_1} + {R_2} = 18\;\Omega \\
\Rightarrow 2\;\Omega + {R_2} = 18\;\Omega \\
\therefore{R_2} = 16\;\Omega
$
Therefore, we obtained that the resistance ${R_1}$ of the aluminium wire is $2\;\Omega $ and the resistance ${R_2}$ of the carbon wire is $16\;\Omega $.
Hence, the option (A) is correct.
Note:The resistance of the individual wires generally changes with the variation in temperature. Since, the resultant resistance of wires in series are considered, we took it as independent of temperature.
Complete step by step answer:
Given:
The temperature coefficient of resistance of aluminium, ${\alpha _{Al}} = 4 \times {10^{ - 3}}\;{\rm{l}}^\circ {\rm{C}}$
The temperature coefficient of resistance of carbon, ${\alpha _C} = 0.5 \times {10^{ - 3}}\;{\rm{l}}^\circ {\rm{C}}$
The resistance of aluminium wire is${R_1}$ .
The resistance of carbon wire is ${R_2}$ .
When wires of resistances ${R_1}$ and ${R_2}$ are connected in series, we can write the resultant resistance of the wires as
$R = {R_1} + {R_2}$
Here $R$ is the resultant resistance of wires of resistances ${R_1}$ and${R_2}$.
We can substitute $18\;\Omega $ for $R$ in in the above equation, we get
${R_1} + {R_2} = 18\;\Omega $
Let the temperature of the wires are increased by $\Delta T$. Then
The new resistance of the aluminium wire, ${{R_1}^1} = {R_1}\left( {1 + {\alpha _{Al}}\Delta T} \right)$
The new resistance of the carbon wire, ${{R_2}^1} = {R_2}\left( {1 + {\alpha _C}\Delta T} \right)$
When wires of resistances ${{R_1}^1}$ and ${{R_2}^1}$ are connected in series, we can write the resultant resistance of the wires as
${R^1} = {{R_1}^1} + {{R_2}^1}$
Here ${R^1}$ is the resultant resistance of ${{R_1}^1}$ and ${{R_2}^1}$ connected in series.
The resistances of a combination of wires remain the same even if the temperatures of the wires are increased. Hence, we can equate the resistances $R$ and ${R^1}$ to get
$
R = {R^1}\\
{R_1} + {R_2} = {{R_1}^1} + {{R_2}^1}
$
Substituting ${R_1}\left( {1 + {\alpha _{Al}}\Delta T} \right)$ for ${{R_1}^1}$ and ${R_2}\left( {1 + {\alpha _C}\Delta T} \right)$ for${{R_2}^1}$, we get
$
{R_1} + {R_2} = {R_1}\left( {1 + {\alpha _{Al}}\Delta T} \right) + {R_2}\left( {1 + {\alpha _C}\Delta T} \right)\\
\Rightarrow{R_1} + {R_2} = {R_1} + {R_1}{\alpha _{Al}}\Delta T + {R_2} + {R_2}{\alpha _C}\Delta T\\
\Rightarrow{R_2}{\alpha _C}\Delta T = - {R_1}{\alpha _{Al}}\Delta T
$
We can avoid the negative sign in the equation.
So, rewriting the above equation, we get
$\dfrac{{{R_2}}}{{{R_1}}} = \dfrac{{{\alpha _{Al}}}}{{{\alpha _C}}}$
Hence, we obtained an equation in the form of the ratio between ${R_2}$ and${R_1}$ .
Substituting $4 \times {10^{ - 3}}\;{\rm{l}}^\circ {\rm{C}}$ for ${\alpha _{Al}}$ and $0.5 \times {10^{ - 3}}\;{\rm{l}}^\circ {\rm{C}}$ for ${\alpha _C}$ in the above equation, we get
$
\dfrac{{{R_2}}}{{{R_1}}} = \dfrac{{4 \times {{10}^{ - 3}}\;{\rm{l}}^\circ {\rm{C}}}}{{0.5 \times {{10}^{ - 3}}\;{\rm{l}}^\circ {\rm{C}}}}\\
\Rightarrow\dfrac{{{R_2}}}{{{R_1}}} = 8\\
\Rightarrow{R_2} = 8{R_1}
$
Substituting $8{R_1}$ for ${R_2}$ in ${R_1} + {R_2} = 18\;\Omega $, we get
$
{R_1} + 8{R_1} = 18\;\Omega \\
\Rightarrow 9{R_1} = 18\;\Omega \\
\Rightarrow{R_1} = 2\;\Omega
$
Hence, we obtained the value of the resistance of the aluminium wire as$2\;\Omega $.
Substituting $2\;\Omega $ for ${R_1}$ in the equation${R_1} + {R_2} = 18\;\Omega $, we obtain
$
{R_1} + {R_2} = 18\;\Omega \\
\Rightarrow 2\;\Omega + {R_2} = 18\;\Omega \\
\therefore{R_2} = 16\;\Omega
$
Therefore, we obtained that the resistance ${R_1}$ of the aluminium wire is $2\;\Omega $ and the resistance ${R_2}$ of the carbon wire is $16\;\Omega $.
Hence, the option (A) is correct.
Note:The resistance of the individual wires generally changes with the variation in temperature. Since, the resultant resistance of wires in series are considered, we took it as independent of temperature.
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