358761 A parallel plate condenser consists of two circular plates each of radius \(2\;cm\) separated by a distance of \(0.1\;mm\). A time varying potential difference of \(5 \times {10^3}\;V/s\) is applied across the plates of the condenser. The displacement current is

358762 Match the Column I and Column II.
Column I
Column II
A
\(\oint {\overrightarrow E } .d\overrightarrow A = Q/{\varepsilon _0}\)
P
Faraday's law
B
\(\oint {\overrightarrow B } .d\overrightarrow A = 0\)
Q
Ampere-Maxwell law
C
\(\oint {\overrightarrow E } .\overrightarrow {dl} = - \frac{{d{\phi _E}}}{{dt}}\)
R
Gauss law for electricity
D
\(\oint {\overrightarrow E } .\overrightarrow {dl} = {u_0}{i_c}\) \(\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\, + {u_0}{\varepsilon _0}\frac{{d{\phi _E}}}{{dt}}\)
S
Gauss law for magnetism

358763 Statement A :
Displacement current goes through the gap between the plates of a capacitor when the charge of the capacitor does not change.
Statement B :
The displacement current arises in the region in which the electric field is constant with time.

358764 Maxwell's equations describe the fundamental laws of

358765 Displacement current is continuous

358761 A parallel plate condenser consists of two circular plates each of radius \(2\;cm\) separated by a distance of \(0.1\;mm\). A time varying potential difference of \(5 \times {10^3}\;V/s\) is applied across the plates of the condenser. The displacement current is

358762 Match the Column I and Column II.
Column I
Column II
A
\(\oint {\overrightarrow E } .d\overrightarrow A = Q/{\varepsilon _0}\)
P
Faraday's law
B
\(\oint {\overrightarrow B } .d\overrightarrow A = 0\)
Q
Ampere-Maxwell law
C
\(\oint {\overrightarrow E } .\overrightarrow {dl} = - \frac{{d{\phi _E}}}{{dt}}\)
R
Gauss law for electricity
D
\(\oint {\overrightarrow E } .\overrightarrow {dl} = {u_0}{i_c}\) \(\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\, + {u_0}{\varepsilon _0}\frac{{d{\phi _E}}}{{dt}}\)
S
Gauss law for magnetism

358763 Statement A :
Displacement current goes through the gap between the plates of a capacitor when the charge of the capacitor does not change.
Statement B :
The displacement current arises in the region in which the electric field is constant with time.

358764 Maxwell's equations describe the fundamental laws of

358765 Displacement current is continuous

358761 A parallel plate condenser consists of two circular plates each of radius \(2\;cm\) separated by a distance of \(0.1\;mm\). A time varying potential difference of \(5 \times {10^3}\;V/s\) is applied across the plates of the condenser. The displacement current is

358762 Match the Column I and Column II.
Column I
Column II
A
\(\oint {\overrightarrow E } .d\overrightarrow A = Q/{\varepsilon _0}\)
P
Faraday's law
B
\(\oint {\overrightarrow B } .d\overrightarrow A = 0\)
Q
Ampere-Maxwell law
C
\(\oint {\overrightarrow E } .\overrightarrow {dl} = - \frac{{d{\phi _E}}}{{dt}}\)
R
Gauss law for electricity
D
\(\oint {\overrightarrow E } .\overrightarrow {dl} = {u_0}{i_c}\) \(\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\, + {u_0}{\varepsilon _0}\frac{{d{\phi _E}}}{{dt}}\)
S
Gauss law for magnetism

358763 Statement A :
Displacement current goes through the gap between the plates of a capacitor when the charge of the capacitor does not change.
Statement B :
The displacement current arises in the region in which the electric field is constant with time.

358764 Maxwell's equations describe the fundamental laws of

358765 Displacement current is continuous

358761 A parallel plate condenser consists of two circular plates each of radius \(2\;cm\) separated by a distance of \(0.1\;mm\). A time varying potential difference of \(5 \times {10^3}\;V/s\) is applied across the plates of the condenser. The displacement current is

358762 Match the Column I and Column II.
Column I
Column II
A
\(\oint {\overrightarrow E } .d\overrightarrow A = Q/{\varepsilon _0}\)
P
Faraday's law
B
\(\oint {\overrightarrow B } .d\overrightarrow A = 0\)
Q
Ampere-Maxwell law
C
\(\oint {\overrightarrow E } .\overrightarrow {dl} = - \frac{{d{\phi _E}}}{{dt}}\)
R
Gauss law for electricity
D
\(\oint {\overrightarrow E } .\overrightarrow {dl} = {u_0}{i_c}\) \(\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\, + {u_0}{\varepsilon _0}\frac{{d{\phi _E}}}{{dt}}\)
S
Gauss law for magnetism

358763 Statement A :
Displacement current goes through the gap between the plates of a capacitor when the charge of the capacitor does not change.
Statement B :
The displacement current arises in the region in which the electric field is constant with time.

358764 Maxwell's equations describe the fundamental laws of

358765 Displacement current is continuous

358761 A parallel plate condenser consists of two circular plates each of radius \(2\;cm\) separated by a distance of \(0.1\;mm\). A time varying potential difference of \(5 \times {10^3}\;V/s\) is applied across the plates of the condenser. The displacement current is

358762 Match the Column I and Column II.
Column I
Column II
A
\(\oint {\overrightarrow E } .d\overrightarrow A = Q/{\varepsilon _0}\)
P
Faraday's law
B
\(\oint {\overrightarrow B } .d\overrightarrow A = 0\)
Q
Ampere-Maxwell law
C
\(\oint {\overrightarrow E } .\overrightarrow {dl} = - \frac{{d{\phi _E}}}{{dt}}\)
R
Gauss law for electricity
D
\(\oint {\overrightarrow E } .\overrightarrow {dl} = {u_0}{i_c}\) \(\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\, + {u_0}{\varepsilon _0}\frac{{d{\phi _E}}}{{dt}}\)
S
Gauss law for magnetism

358763 Statement A :
Displacement current goes through the gap between the plates of a capacitor when the charge of the capacitor does not change.
Statement B :
The displacement current arises in the region in which the electric field is constant with time.

358764 Maxwell's equations describe the fundamental laws of

358765 Displacement current is continuous