Explanation
Consider a cube as shown in the fig-1; with uniformly distributed charge within its volume. The potential at one of its vertex P is {V_0}.A cubical portion of half the size (half edge length) of the original cube is cut and removed as shown in the fig-Find the modulus of potential at the point P in the new structure.
A potentiometer has a wire of 100 cm length and its resistance is 10 ohms. It is connected in series with a resistance of 40 ohms and a battery of emf 2 V and negligible internal resistance. If a source of unknown emf E connected in the secondary is balanced by 40 cm length of potentiometer wire, the value of E is:
For the following circuits, the potential difference betweenX and Y in volt is \left( {{V_x} - {V_y}} \right)
\textbf{Step1: Slope of $$V-I$$ graph}
Ohm's Law states that V=IR
So, \dfrac{{{V}_{1}}}{{{I}_{1}}}\ =\tan \theta \ = \ {{R}_{1}}
\& \dfrac{{{V}_{2}}}{{{I}_{2}}}\ =\tan (90-\theta )\ =\cot \theta \ =\ {{R}_{2}}
\textbf{Step2: Calculation of} T_2 -T_1
Temperature dependence of resistance is given by:
R_1 = R_0(1+\alpha T_1)
R_2 = R_0(1+\alpha T_2)
Subtracting above equations, we get
R_2-R_1 = \alpha(T_2-T_1)
\therefore T_2-T_1 is proportional to R_2-R_1
\Rightarrow {{T}_{2}}-{{T}_{1}}\ \propto \ \left( \cot \theta -\tan \theta \right)=\dfrac{\cos \theta }{\sin \theta }-\dfrac{\sin \theta }{\cos \theta }=\dfrac{{{\cos }^{2}}\theta -{{\sin }^{2}}\theta }{\sin \theta \cos \theta }
{{T}_{2}}-{{T}_{1}}\ \propto \ \dfrac{2\ \cos 2\theta }{\sin 2\theta }\ =\ 2\cot 2\theta
Hence, {{T}_{2}}-{{T}_{1}}\ \propto \ \cot 2\theta
Therefore, Option C is correct
Length of potentiometer wire l=1\,m
Emf e={{E}_{1}}
Emf of cell {{E}_{2}}=1.02\,v/s
Null point =51\,cm=0.51\,m
(a)Potential gradient of the wire
V=\dfrac{1.02}{0.51}
V=2\,V/m
(b) Emf of cell
{{V}_{PQ}}={{E}_{1}}
{{E}_{1}}=2\,V
(c) When switch S is closed, null point does not shifts because current if not drawn from E2 again.
A circular coil of area 8{m^2} and number of turns 20 is placed in a magnetic field of 2T with its plane perpendicular to it. It is rotated with an angular velocity of 20rev/s about its natural axis. The emf induced is
Given,
Resistance become R=3{{R}_{o}}
R={{R}_{0}}\left( 1+\alpha \Delta T \right)
3{{R}_{o}}={{R}_{o}}\left( 1+\alpha \Delta T \right)
\Delta T=\dfrac{2}{\alpha }=\dfrac{2}{4\times {{10}^{-3}}}=500{{\,}^{o}}C
Hence, when rise in temperature is 500{{\,}^{o}}C
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