The physics of non-uniform conductors is a classic test of how well you understand the continuity of charge and the microscopic mechanisms of electric current. Let's dive into the elegant relationship between geometry, electric fields, and the speed of electrons!
The Setup
A Funnel for Electrons
Imagine you are watering your garden with a hose. If you pinch the end of the hose, the water shoots out faster. Why? Because the total volume of water flowing through the hose every second must remain constant. If the opening is smaller, the water must speed up to get through in time.
This exact same principle applies to our conductor PQ. The battery establishes a steady state, meaning charge cannot pile up anywhere inside the material. The total electric current I—the number of coulombs passing through any cross-section per second—must be perfectly constant from end P to end Q.
The Microscopic View
Slicing the Conductor
To understand what happens inside, let's take a microscopic slice of the conductor with a tiny length dl and a local radius r.
The resistance of this tiny element is given by the standard formula:
dR=Aρdl=πr2ρdl
According to Ohm's law, the potential drop
dV across this microscopic slice is simply the current multiplied by this resistance:
dV=IdR=πr2Iρdl
The Master Equation
Electric Field and Radius
Now, we need to find the electric field
E driving the electrons. The electric field is the potential gradient—the rate at which voltage drops over distance:
E=dldV
Substituting our expression for
dV, the
dl beautifully cancels out:
E=πr2Iρ
Look closely at this master equation. The current I is constant, and the resistivity ho is a fixed property of the material. Therefore, the electric field is inversely proportional to the square of the radius (E∝r21). As the conductor narrows, the electric field intensifies!
The Grand Finale
Drift Velocity in Action
Finally, how does this affect the electrons? The drift velocity
vd of an electron is determined by the electric field accelerating it, balanced by collisions with the atomic lattice:
vd=meEτ
This tells us that vd∝E.
As we move from P to Q, the radius r decreases. A smaller radius creates a much stronger electric field. This intensified electric field exerts a greater force on the free electrons, causing their drift velocity vd to increase.
Pro-Tip: You can also solve this instantly using Current Density (J). Since J=AI, a smaller area means a higher J. Because E=ρJ and vd=neJ, both the electric field and drift velocity must increase as the area shrinks!