Know that electrical energy is transferred to heat energy and other forms of energy in the resistor, or other circuit components, and then into the surroundings

Published by Patrick Mutisya · 14 days ago

Cambridge IGCSE Physics 0625 – 4.2.4 Resistance

4.2.4 Resistance

Objective

Understand that electrical energy is converted into heat energy (and sometimes other forms of energy) in a resistor or other circuit component, and that this energy is then transferred to the surroundings.

1. Energy conversion in a resistor

When a current \$I\$ flows through a resistor of resistance \$R\$, the electrical energy supplied by the source is dissipated in the resistor. The main form of this dissipated energy is heat, but in some components (e.g., a filament lamp) part of the energy is emitted as light.

Suggested diagram: A simple circuit showing a battery, a resistor, and arrows indicating the flow of electrical energy into the resistor and heat out to the surroundings.

2. Power dissipated in a resistor

The rate at which electrical energy is converted to heat is called the power \$P\$ of the resistor. The following equivalent expressions are used in IGCSE:

FormulaWhen to use
\$P = VI\$Known voltage across and current through the resistor
\$P = I^{2}R\$Known current and resistance
\$P = \frac{V^{2}}{R}\$Known voltage and resistance

All three forms give the same result because \$V = IR\$ (Ohm’s law).

3. Energy transferred to the surroundings

The energy \$E\$ transferred in a time \$t\$ is:

\$E = Pt\$

Since \$P\$ is usually expressed in watts (J s⁻¹), \$E\$ will be in joules (J) when \$t\$ is in seconds.

4. Factors influencing the amount of heat produced

  • Current (\$I\$): Heat varies with the square of the current (\$P \propto I^{2}\$). Doubling the current increases the heat fourfold.
  • Resistance (\$R\$): For a given current, heat is directly proportional to resistance (\$P \propto R\$). For a given voltage, heat is inversely proportional to resistance (\$P \propto 1/R\$).
  • Time (\$t\$): Longer operation means more total energy transferred.
  • Material and dimensions: Resistivity, length, and cross‑sectional area determine \$R\$ (see Section 5).

5. Calculating resistance

Resistance of a uniform conductor is given by:

\$R = \rho \frac{L}{A}\$

where \$\rho\$ is the resistivity of the material (Ω m), \$L\$ is the length (m), and \$A\$ is the cross‑sectional area (m²).

6. Example calculation

  1. A 10 Ω resistor has a current of 2 A flowing through it. Find the power dissipated and the energy released in 5 minutes.
  2. Solution:

    • Power: \$P = I^{2}R = (2\ \text{A})^{2}\times10\ \Omega = 40\ \text{W}\$
    • Time: \$t = 5\ \text{min}=300\ \text{s}\$
    • Energy: \$E = Pt = 40\ \text{W}\times300\ \text{s}=12\,000\ \text{J}\$

7. Summary of key points

  • Electrical energy is converted to heat (and sometimes light) in resistors.
  • Power dissipated can be calculated using \$P=VI\$, \$P=I^{2}R\$, or \$P=V^{2}/R\$.
  • The total energy transferred to the surroundings is \$E = Pt\$.
  • Heat production increases with the square of the current and is directly proportional to resistance for a given current.
  • Resistivity and the geometry of a conductor determine its resistance.

8. Practice questions

  1. A 5 Ω heater is connected to a 12 V supply. Calculate:

    • The current through the heater.
    • The power it dissipates.
    • The energy released after 10 minutes.

  2. A copper wire (resistivity \$1.68\times10^{-8}\ \Omega\!\cdot\!m\$) is 2 m long and has a cross‑sectional area of \$1.0\times10^{-6}\ \text{m}^{2}\$. Find its resistance and the power dissipated when a current of 3 A flows through it.
  3. Explain why a filament lamp gets hotter than a metal heating element of the same resistance when both are connected to the same voltage source.