358595
Assertion :
In electric circuits, wires carrying currents in opposite directions are often twisted together.
Reason :
If the wires are not twisted together, the combination of wires forms a current loop. The magnetic field generated by the loop might affect adjacent circuits or components.
358597
In the figure as shown, a conducting wire \({P Q}\) of length \(1\,m\) is moving in a uniform magnetic field \({B=3 {~T}}\) with constant velocity \({v=2 {~m} / {sec}}\) towards right. Given, \(R = 2\,\Omega \), \({C=1 {~F}}\) and \(L = 2\,H\). The current through resistance, capacitor and inductor at any time \({t}\) are \({I_{1}, I_{2}}\) and \({I_{3}}\) respectively. The value of \({I_3}\) at time \(t = 2\,\sec \) is
358595
Assertion :
In electric circuits, wires carrying currents in opposite directions are often twisted together.
Reason :
If the wires are not twisted together, the combination of wires forms a current loop. The magnetic field generated by the loop might affect adjacent circuits or components.
358597
In the figure as shown, a conducting wire \({P Q}\) of length \(1\,m\) is moving in a uniform magnetic field \({B=3 {~T}}\) with constant velocity \({v=2 {~m} / {sec}}\) towards right. Given, \(R = 2\,\Omega \), \({C=1 {~F}}\) and \(L = 2\,H\). The current through resistance, capacitor and inductor at any time \({t}\) are \({I_{1}, I_{2}}\) and \({I_{3}}\) respectively. The value of \({I_3}\) at time \(t = 2\,\sec \) is
358595
Assertion :
In electric circuits, wires carrying currents in opposite directions are often twisted together.
Reason :
If the wires are not twisted together, the combination of wires forms a current loop. The magnetic field generated by the loop might affect adjacent circuits or components.
358597
In the figure as shown, a conducting wire \({P Q}\) of length \(1\,m\) is moving in a uniform magnetic field \({B=3 {~T}}\) with constant velocity \({v=2 {~m} / {sec}}\) towards right. Given, \(R = 2\,\Omega \), \({C=1 {~F}}\) and \(L = 2\,H\). The current through resistance, capacitor and inductor at any time \({t}\) are \({I_{1}, I_{2}}\) and \({I_{3}}\) respectively. The value of \({I_3}\) at time \(t = 2\,\sec \) is
358595
Assertion :
In electric circuits, wires carrying currents in opposite directions are often twisted together.
Reason :
If the wires are not twisted together, the combination of wires forms a current loop. The magnetic field generated by the loop might affect adjacent circuits or components.
358597
In the figure as shown, a conducting wire \({P Q}\) of length \(1\,m\) is moving in a uniform magnetic field \({B=3 {~T}}\) with constant velocity \({v=2 {~m} / {sec}}\) towards right. Given, \(R = 2\,\Omega \), \({C=1 {~F}}\) and \(L = 2\,H\). The current through resistance, capacitor and inductor at any time \({t}\) are \({I_{1}, I_{2}}\) and \({I_{3}}\) respectively. The value of \({I_3}\) at time \(t = 2\,\sec \) is
358595
Assertion :
In electric circuits, wires carrying currents in opposite directions are often twisted together.
Reason :
If the wires are not twisted together, the combination of wires forms a current loop. The magnetic field generated by the loop might affect adjacent circuits or components.
358597
In the figure as shown, a conducting wire \({P Q}\) of length \(1\,m\) is moving in a uniform magnetic field \({B=3 {~T}}\) with constant velocity \({v=2 {~m} / {sec}}\) towards right. Given, \(R = 2\,\Omega \), \({C=1 {~F}}\) and \(L = 2\,H\). The current through resistance, capacitor and inductor at any time \({t}\) are \({I_{1}, I_{2}}\) and \({I_{3}}\) respectively. The value of \({I_3}\) at time \(t = 2\,\sec \) is