Sigma Percentile
JEE Advanced 1997
LEVELJEE Main

Animated Solution for Physics - Current Electricity: A steady current flows in a metallic conductor of non-uniform cross-section. The quantity/quantities constant along the length of the conductor is/are

Select Answer:

Visualized Solution

  • For a steady current flowing through a conductor, the rate of flow of charge across any cross-section is constant.

  • The drift velocity is related to current by the equation , where is the electron density, is the elementary charge, and is the cross-sectional area.

  • Since , , and are constant, . As the area changes, the drift velocity must change.

  • From Ohm's law, , where . Thus, .

\text{Conclusion}

  • Only the current remains constant along the length of the non-uniform conductor.

\text{The Way Forward}

  • What if the current was not steady? In a transient state, charge could accumulate at certain cross-sections, making variable.

The Sigma Insight: Ohm's Law, Resistance and Electrical Power

Solution Diagram

The Steady Flow of Charge

Imagine a river flowing through a canyon. In some places, the river is wide and lazy, and in others, it narrows into roaring rapids. But if the flow is steady, the total volume of water passing any point every second must be exactly the same. If it weren't, water would magically appear or disappear!
The exact same principle applies to electric current. A steady current means that the rate of flow of charge is constant over time. Therefore, the current must be identical at every cross-section of the conductor, regardless of whether the wire is thick or thin. This is a direct consequence of the conservation of charge.

The Microscopic View

Drift Velocity
Now, let's zoom in and look at the electrons. The relationship between the macroscopic current and the microscopic drift velocity is given by the famous equation:
Here, is the number density of free electrons (which depends only on the material), is the elementary charge, and is the cross-sectional area.
Since , , and are all constants in our scenario, we can easily see how drift velocity behaves:
This tells us that drift velocity is inversely proportional to the cross-sectional area. Where the conductor is wide, the electrons can afford to drift slowly. But when the conductor narrows, the electrons must speed up to maintain that constant flow of charge—just like the water in the narrow rapids!

The Driving Force

Electric Field
What causes the electrons to speed up in the narrow sections? It's the electric field! We can understand this using the microscopic form of Ohm's Law:
Where is the current density () and is the conductivity of the material. Substituting into the equation gives us:
Because and are constant, we find that:
The electric field is also inversely proportional to the cross-sectional area. In the narrow regions, the electric field must be stronger to push the electrons faster and maintain the steady current.

The Final Verdict

By analyzing the physics, we've discovered a beautiful interplay of variables. While the drift speed and the electric field constantly adjust themselves to the changing geometry of the wire, the current remains the unwavering constant throughout the entire journey.

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