Charges experience an electric field and move accordingly. In a typical metal, each atom in the lattice will allow one of its electrons to move freely. So the metal can be thought of as a rigid lattice of positively-charged ion cores surrounded by a swarm of free electrons. Later in the semester we will see how the Hall effect demonstated that electrons are in fact the free charge carriers in simple metals.
Do the electrons accelerate indefinitely because of the applied potential? NO, on average they reach a terminal speed, much as a skydiver reaches a terminal velocity of about 120mph falling through air, a viscous medium. The electrons tend to drift slowly through the conductor, on the order of 0.01 mm/s. The "viscosity" that the electrons experience is called resistance. Many conductors are referred to simply as resistors.
But what about the speed of propagation? Many of you know that electronic signals propagate near the speed of light. For example, the bits coming to this computer via the Ethernet travel at about 0.8 times the speed of light. We will examine this more fully very near the end of the semester.
For the time being you may think of the "water in hose" analogy. When the valve to a garden hose is opened, water "immediately" leaves the end of the hose. However the water actually passing through the valve takes much longer to reach the end of the hose. Here the pressure wave that propagates at the speed of sound in water would represent the electronic signal.
Also please keep in mind that although that electrons are flowing through the conductor, there is no charge accumulation anywhere. The electrons flow in a continuous loop, known as a circuit. The electrons are continuously flowing past the positively-charged ion cores, with no change in the net charge anywhere. See animation below:
So the result of a voltage difference across a resistor is that electric current flows. Precisely, current is the instantaneous rate at which charge passes through a cross-section of the conductor.
We will start with the study of steady currents, the so-called direct current, or dc for short. Later in the semester, we will study RC circuits and their decaying transient currents, followed by alternating (or ac) circuits.
The unit of resistance is volt/amp, known as an ohm, and represented by upper case omega.
The resistance of a conductor depends on material and geometry. These effects may be separated by considering the resistivity of the material.
Refer to the Play-Doh Experiment
rho is the resistivity of the conductor, a material property, not a geometrical one. There is a wide range of resistivities available, from as low as 10^-8 ohm-m for pure metals to as high as 10^17 ohm-m for an excellent insulator.
Resistance controls the amount of current that results when voltage difference is applied to a resistor.
If a material obeys the relationship above it is said to be ohmic. Not all materials are ohmic, and fortuately so, else we wouldn't have the wonderful semiconductor-based devices to which we have become so accustomed.
|To the chalkboard for presentation of first simple circuit and derivation of Joule's law.|
Last updated Sept. 12, 1997.
Copyright George Watson, Univ. of Delaware, 1997.