A lightbulb filament is a very thin tungsten wire that is heated until it glows by passing a current through it.
In This Chapter, you will learn how and why charge moves through a wire as a current.
Current is the flow of charge through a conductor. We can’t see charge moving, but two indicators of current are:
A nearby compass needle is deflected.
A wire with a current gets warm.
Current is measured in amperes, a charge flow rate of one coulomb per second. You know this informally as “amps.”
《 LOOKING BACK Section 23.6 The motion of charges in electric fields
We’ll develop a model of conduction:
Connecting a wire to a battery causes a nonuniform surface charge distribution.
The surface charges create an electric field inside the wire.
The electric field pushes the sea of electrons through the metal.
Electrons are the charge carriers in metals, but it is customary to treat current as the motion of positive charges.
Current is . Current density is the amount of current per square meter.
Current is governed by Kirchhoff’s junction law.
The current is the same everywhere in a circuit with no junctions.
The sum of currents entering a junction equals the sum leaving.
Collisions of electrons with atoms cause a conductor to resist the motion of charges.
Resistivity is an electrical property of a material, such as copper.
Resistance is a property of a specific wire or circuit element based on the material of which it is made and its size and shape.
Ohm’s law says that the current flowing through a wire or circuit element depends on both the potential difference across it and the element’s resistance:
《 LOOKING BACK Section 26.4 Sources of potential
After studying this chapter, you should be able to
27.1 Explain the motion of charged particles through a conductor.
27.2 Apply a statistical model of conduction.
27.3 Calculate current as the rate of flow of charge.
27.4 Use conductivity and resistivity to relate current and current density.
27.5 Apply Ohm’s law to simple circuits with one resistor.