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Current and Resistance: Study Notes for Physics Students

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Current and Resistance

Charge Carriers in Metals

In metallic conductors, the outer electrons of atoms are only weakly bound to their nuclei. These electrons become detached and form a 'sea' of conduction electrons, which are free to move throughout the solid. The movement of these electrons underlies the concept of electric current in metals.

  • Conduction electrons are responsible for carrying charge in metals.

  • The metal as a whole remains electrically neutral, with positive ions fixed in place and electrons free to move.

Sea of electrons in a metal

The Electron Current

The electron current () is defined as the number of electrons passing through a cross-section of a conductor per second. If electrons pass through in a time interval , then:

  • If the number density of conduction electrons is , the total number of electrons in a segment of wire of cross-sectional area and length is .

  • Since (where is the drift speed), .

  • Thus,

Electron current through a wireElectrons moving through a wire at drift speedVolume of electrons moving in a wire

Electron Density in Metals

Each atom in a metal typically contributes one conduction electron. The number density is thus approximately equal to the number of atoms per cubic meter. Typical values for common metals are:

Metal

Electron Density ( m)

Aluminum

18

Iron

17

Copper

8.5

Gold

5.9

Silver

5.8

Example: Calculating Electron Current

For a 2.0-mm-diameter copper wire with electron drift speed m/s and m:

  • Cross-sectional area: m

  • Electron current: electrons/s

Discharging a Capacitor

Although the drift speed of electrons is slow, capacitors discharge almost instantaneously because the wire is already full of electrons. Discharging involves only a slight rearrangement of charges, not the movement of individual electrons from one plate to another.

Capacitor discharge through a wireElectron movement during capacitor discharge

Creating and Sustaining a Current

To maintain a steady current, a continuous 'push' is needed, analogous to pushing a book across a table against friction. In conductors, this push is provided by an electric field.

Analogy between pushing a book and moving electrons

Establishing the Electric Field in a Wire

When two wires are connected to the plates of a charged capacitor, surface charges rearrange almost instantly, creating a nonuniform distribution. This distribution establishes an internal electric field that drives the electron current.

Initial state: no current, uniform surface chargeNonuniform surface charge after connectionElectric field from nonuniform surface charge

Direction of Electron Drift

The internal electric field points from the more positive to the more negative end of the wire, causing electrons (negative charge carriers) to drift in the opposite direction.

Surface charge distribution and electron driftDirection of electron drift

A Model of Conduction

In electrostatic equilibrium (no electric field), electrons move randomly and have zero average velocity. When an electric field is present, electrons follow curved paths between collisions, resulting in a slow net drift opposite to the field.

Electron motion with no electric fieldElectron motion with an electric fieldGraph of electron speed during collisions

Electron Current and Electric Field

The electric field in a wire of cross-section causes an electron current:

  • Here, is the mean time between collisions, and is the electron mass.

  • The electron current is directly proportional to the electric field strength.

Current and Conventional Current

The total current is the rate at which charge flows through a wire:

  • SI unit: ampere (A), where

  • The direction of conventional current is opposite to the direction of electron flow in metals.

Direction of current and electron current

Current Density

The current density is the current per unit area:

  • Units: A/m

Resistance and Ohm's Law

The resistance of a conductor is defined as:

  • , where is the resistivity, is the length, and is the cross-sectional area.

  • The current through a conductor is proportional to the potential difference across it: (Ohm's Law).

  • Unit of resistance: ohm (), where

Potential difference and current in a conductor

Ohmic and Nonohmic Materials

Materials that obey Ohm's law (constant ) are called ohmic. For these materials, the current is directly proportional to the potential difference. Nonohmic materials (e.g., diodes, batteries, capacitors) do not have a constant resistance, and their - relationship is nonlinear.

Ohmic material: linear I-V relationshipNonohmic material: nonlinear I-V relationship

Batteries and Circuits

A battery provides a potential difference that drives current through a circuit. The current in a simple battery-wire-resistor circuit is the same at all points, and is given by .

Battery and resistor in a circuitCurrent in a battery-resistor circuit

Summary Table: Key Equations

Quantity

Equation

Units

Electron current

electrons/s

Current

A (C/s)

Current density

A/m

Resistance

Ohm's Law

A

Additional info: These notes cover the fundamental concepts of electric current, electron flow, current density, resistance, Ohm's law, and the behavior of ohmic and nonohmic materials, as well as the role of batteries in circuits. The included images reinforce the physical models and equations described.

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