
A condenser of capacity \[{C_1}\] is charged to a potential \[{V_0}.\] The electrostatic energy stored in it is \[{U_0}.\] It is connected to another uncharged condenser of capacity \[{C_2}\]in parallel. The energy dissipated in the process is:
A. $\dfrac{{{C_2}}}{{{C_1} + {C_2}}}{U_0}$
B. $\dfrac{{{C_1}}}{{{C_1} + {C_2}}}{U_0}$
C. $(\dfrac{{{C_1} - {C_2}}}{{{C_1} + {C_2}}}){U_0}$
D. $\dfrac{{{C_1}{C_2}}}{{2({C_1} + {C_2})}}{U_0}$
Answer
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Hint: To solve this question, we will start with taking the initial energy and initial charge of condenser \[{C_1}.\] Now, it is given that condenser \[{C_1}\]is connected parallelly to another uncharged condenser of capacity \[{C_2}.\] So, now we will take the total energy and total charge of the system. Then we will evaluate the energy dissipated in the whole process.
Complete step by step answer:
We have been given a condenser of capacity \[{C_1}\] which is charged to a potential \[{V_0}.\]The electrostatic energy stored in it is \[{U_0}.\]The given condenser is connected to another uncharged condenser of capacity \[{C_2}\] in parallel. We need to find the energy dissipated in the process.
So, given potential of a condenser of capacity \[{C_1} = {\text{ }}{V_0}\]
Also given the electrostatic energy stored in condenser \[ = {\text{ }}{U_0}\]
At first, we will get the initial energy of the condenser \[{C_1}\] by applying the formula mentioned below.
Initial energy, \[{U_i}\] $ = \dfrac{{QV}}{2} = \dfrac{{C{V^2}}}{2}$
where, Q \[ = \] charge
V \[ = \] potential
C \[ = \] condenser
So, on putting the value in the above-mentioned formula, we get
The initial energy of condenser\[{C_{1,}}\] \[{U_i} = {U_0} = \dfrac{1}{2}{C_1}{V_0}^2\]
And the initial charge of the system, ${Q_i} = {C_1}{V_0}$
Now, it is given that condenser \[{C_1}\]connected parallelly to another uncharged condenser of capacity \[{C_2}.\]
So, after connecting another condenser, the final charge of both \[{C_1}\] and \[{C_2}\],\[\]${Q_f} = ({C_1} + {C_2}){V_c}$
where, ${V_c} = $ common potential after connecting.
As total charge is conserved, ${Q_i} = {Q_f} = {C_1}{V_0} = ({C_1} + {C_2}){V_c}$
$\therefore {V_c} = \dfrac{{{C_1}{V_0}}}{{({C_1} + {C_2})}}$
Now, the final energy, ${U_f} = \dfrac{1}{2}({C_1} + {C_2}){V_c}^2$
$ = \dfrac{1}{2}({C_1} + {C_2}){\left( {\dfrac{{{C_1}{V_0}}}{{{C_1} + {C_2}}}} \right)^2} = \dfrac{{{C_1}{U_0}}}{{{C_1} + {C_2}}}$
Hence, the energy dissipation $ = {U_i} - {U_f}$
$ = {U_0} - \dfrac{{{C_1}{U_0}}}{{{C_1} + {C_2}}}$
$ = \dfrac{{{C_2}{U_0}}}{{{C_1} + {C_2}}}$
So, the correct answer is “Option A”.
Note:
In the question above we have been asked about the energy dissipation. So, energy is dissipated, when there is a change in a system, the energy gets transferred and in that process some of that energy is dissipated or wasted. We can say the energy gets lost to the surroundings.
Complete step by step answer:
We have been given a condenser of capacity \[{C_1}\] which is charged to a potential \[{V_0}.\]The electrostatic energy stored in it is \[{U_0}.\]The given condenser is connected to another uncharged condenser of capacity \[{C_2}\] in parallel. We need to find the energy dissipated in the process.
So, given potential of a condenser of capacity \[{C_1} = {\text{ }}{V_0}\]
Also given the electrostatic energy stored in condenser \[ = {\text{ }}{U_0}\]
At first, we will get the initial energy of the condenser \[{C_1}\] by applying the formula mentioned below.
Initial energy, \[{U_i}\] $ = \dfrac{{QV}}{2} = \dfrac{{C{V^2}}}{2}$
where, Q \[ = \] charge
V \[ = \] potential
C \[ = \] condenser
So, on putting the value in the above-mentioned formula, we get
The initial energy of condenser\[{C_{1,}}\] \[{U_i} = {U_0} = \dfrac{1}{2}{C_1}{V_0}^2\]
And the initial charge of the system, ${Q_i} = {C_1}{V_0}$
Now, it is given that condenser \[{C_1}\]connected parallelly to another uncharged condenser of capacity \[{C_2}.\]
So, after connecting another condenser, the final charge of both \[{C_1}\] and \[{C_2}\],\[\]${Q_f} = ({C_1} + {C_2}){V_c}$
where, ${V_c} = $ common potential after connecting.
As total charge is conserved, ${Q_i} = {Q_f} = {C_1}{V_0} = ({C_1} + {C_2}){V_c}$
$\therefore {V_c} = \dfrac{{{C_1}{V_0}}}{{({C_1} + {C_2})}}$
Now, the final energy, ${U_f} = \dfrac{1}{2}({C_1} + {C_2}){V_c}^2$
$ = \dfrac{1}{2}({C_1} + {C_2}){\left( {\dfrac{{{C_1}{V_0}}}{{{C_1} + {C_2}}}} \right)^2} = \dfrac{{{C_1}{U_0}}}{{{C_1} + {C_2}}}$
Hence, the energy dissipation $ = {U_i} - {U_f}$
$ = {U_0} - \dfrac{{{C_1}{U_0}}}{{{C_1} + {C_2}}}$
$ = \dfrac{{{C_2}{U_0}}}{{{C_1} + {C_2}}}$
So, the correct answer is “Option A”.
Note:
In the question above we have been asked about the energy dissipation. So, energy is dissipated, when there is a change in a system, the energy gets transferred and in that process some of that energy is dissipated or wasted. We can say the energy gets lost to the surroundings.
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