Physics Current Electricity 3 Marks
Appeared in: 2024 (2 sets)
(a) Define ‘current density’. Is it a scalar or a vector ? An electric field $\vec{E}$ is maintained in a metallic conductor. If $n$ be the number of electrons (mass $m$, charge $-e$) per unit volume in the conductor and $\tau$ its relaxation time, show that the current density $\vec{j} = \alpha \vec{E}$, where $\alpha = \left$ \frac{ne^2}{m} \right$ \tau$. OR (b) What is a Wheatstone bridge ? Obtain the necessary conditions under which the Wheatstone bridge is balanced.
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Solution (a)

Step 1 (Definition and Nature): [0.5 Mark]

Current density ($\vec{j}$) is defined as the amount of electric current flowing per unit area of cross-section held normal to the direction of the current. It is a vector quantity.

Mathematically: $\vec{j} = \frac{I}{A} \hat{n}$

Step 2 (Mathematical Derivation): [2 Marks]

  • The drift velocity ($\vec{v}_d$) of electrons in an electric field $\vec{E}$ is given by: $$\vec{v}_d = -\frac{e\vec{E}}{m}\tau$$
  • The relation between current density ($\vec{j}$) and drift velocity ($\vec{v}_d$) is: $$\vec{j} = -ne\vec{v}_d$$
  • Substituting the expression for $\vec{v}_d$ into the equation for $\vec{j}$: $$\vec{j} = -ne \left( -\frac{e\vec{E}}{m}\tau \right)$$
  • Simplifying the expression: $$\vec{j} = \left( \frac{ne^2\tau}{m} \right) \vec{E}$$

Step 3 (Final Conclusion): [0.5 Mark]

Comparing the derived expression with $\vec{j} = \alpha \vec{E}$, we get:

$$\alpha = \frac{ne^2\tau}{m}$$

This constant $\alpha$ is known as the electrical conductivity ($\sigma$) of the material.


💡 EL10 Concept Insight

Think of current density as the "crowd flow" of electrons: just like more people passing through a gate per second means a higher flow, the electric field acts like a push that accelerates electrons, while the relaxation time is the average time they can "run" before bumping into atoms and slowing down.

Solution (b)

Step 1 (Definition): [0.5 Mark]

A Wheatstone bridge is an electrical circuit used to measure an unknown resistance by balancing two legs of a bridge circuit, one leg of which includes the unknown component.

Step 2 (Mathematical Working - Kirchhoff's Laws): [2 Marks]

  • Consider a bridge with resistors $P, Q, R, S$ and a galvanometer $G$. Applying Kirchhoff’s Junction Rule at nodes B and D:
    At node B: $I_1 - I_g - I_3 = 0$
    At node D: $I_2 + I_g - I_4 = 0$
  • Applying Kirchhoff’s Loop Rule to loop ABDA: $$-I_1P - I_gG + I_2R = 0$$
  • For a balanced bridge, the galvanometer shows no deflection, so $I_g = 0$. The equations become:
    $I_1 = I_3$ and $I_2 = I_4$
    $-I_1P + I_2R = 0 \implies I_1P = I_2R$
  • Applying Kirchhoff’s Loop Rule to loop BCDB: $$-I_3Q + I_4S + I_gG = 0$$ Since $I_g = 0$, then $I_3Q = I_4S$.