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9. Electricity

Written by: Pranav I
Formatted by: Adhulan Rajkamal

Index

9.1 Electric current

  • Electric current: flow of charge carriers
  • \( e = -1.60 \times 10^{-19} \) C (coulomb: unit of charge)
  • Charge is quantised → integral multiples of \( e \)
  • Free electrons move throughout a metal; drift towards the +ve terminal when a battery is connected across its ends
  • Unit of current → ampere
  • \( Q = It \) (charge = current × time)

Conventional Current

  • In the direction of flow of positive charge; from the positive terminal to the negative terminal
  • Electron flow: in the direction of the flow of electrons (opposite to conventional current); from the negative terminal to the positive terminal

Conduction in a Current-Carrying Conductor

  • \( I = Anvq \)
    • \( I \) is current
    • \( A \) is cross-sectional area of the conductor
    • \( n \) is the number density of the charge carriers
    • \( v \) is the average drift speed
    • \( q \) is the charge per charge carrier

9.2 Potential difference and power

  • Energy transferred per unit charge (more specific definitions in Chapter 10)
  • Unit of potential difference → volt (V)
  • \( V = \frac{W}{Q} \) (p.d is the work done by a unit charge moving between two points in a circuit)
    • Present ‘across the ends of a device’

Electrical Power

  • \( P = VI \) (power = potential difference × current)
  • Unit of power → watt (W)

9.3 Resistance and resistivity

  • Good conductors – low resistance; bad conductors (insulators) – high resistance
  • \( R = \frac{V}{I} \) (potential difference / current)
  • Unit of resistance → ohm (\(\Omega\))
  • Controls the flow of current
    • For a given p.d, high resistance means a small current, and vice versa

Electrical heating

  • Joule heating occurs when an electric current passes through a resistor
  • \( P = I^2 R \) and \( P = \frac{V^2}{R} \)

Current-voltage (I-V) characteristics

Circuit used for taking I and V readings
I-V characteristic of a conductor (e.g. constantan wire)
  • Resistance (and temperature) remains constant throughout
I-V characteristic of a filament lamp
  • Resistance is constant at first, but then increases with current as the temperature increases 

Ohm’s Law

  • The current through a conductor is directly proportional to the potential difference across the conductor provided that the temperature of the conductor remains constant 

Electrical heating

I-V characteristic of a diode

  • Allows current to flow in one direction only (in forward bias; not in reverse bias)
  • Very high resistance for low voltages in forward bias
  • Resistance decreases as the voltage is increased

Resistance and temperature

  • The higher the temperature, the greater the amplitude of vibration of metal ions
  • Collisions of electrons with vibrating metal ions impede their movement (resistance)
  • Greater chances of collision at higher temperatures
  • Heating is caused by the transfer of energy from electrons to metal ions on collision
  • ∴ As current increases, temperature increases and resistance increases

Resistivity

  • \( R \propto L \)
  • \( R \propto \frac{1}{A} \)
  • R also depends on the type of material
    • \( \rho \) → resistivity (for a material; at a temperature)
    • Unit of resistivity → ohm metre (\(\Omega \text{m}\))
  • \( R = \frac{\rho L}{A} \) (note: A is the cross-sectional area)
  • Resistivity increases with increasing temperature in metals
  • Resistivity rapidly decreases with increasing temperature in semiconductors

The light-dependent resistor (LDR)

  • As the light intensity increases, the resistance of the LDR decreases

The thermistor

  • Negative temperature coefficient (NTC) device
  • Made from semiconducting material
  • As the temperature increases, the resistance of the thermistor decreases significantly
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