11. Temperature (A-level) Notes (Thermal Equilibrium, Scales, and Thermometers)

11.1 Thermal Equilibrium

  • Thermal energy flows from an area of higher temperature to an area of lower temperature when objects are in thermal contact.
  • Energy transfer continues until the objects reach the same temperature, i.e., thermal equilibrium.
  • Zeroth law of thermodynamics: if object A is in thermal equilibrium with object B, and object B is in thermal equilibrium with object C, then A is in thermal equilibrium with C.
  • Practical implication: thermal equilibrium defines a common temperature reference for connected bodies; energy exchange ceases when equilibrium is reached.

11.2 Temperature Scales

  • Many physical properties vary with temperature and can be used to measure temperature, such as:
    • Change in resistance of a metallic conductor or semiconductor (e.g., thermistor).
    • Voltage produced across a thermocouple.
    • Change in volume of a liquid.
    • Change in volume of a gas at constant pressure.
    • Change in pressure of a gas at constant volume.
  • Kelvin scale (thermodynamic temperature scale): the Kelvin scale is an absolute scale that does not depend on the property of any substance.
  • Celsius scale: depends on the melting point (0° C) and boiling point (100° C) of pure water at atmospheric pressure.
  • Absolute zero: 0 K on the Kelvin scale; the temperature at which particles have no kinetic energy and the volume and pressure of a gas would be zero.
  • All equations in thermal physics use temperature measured in kelvin (K).
  • A change of 1 K is equal to a change of 1 °C, i.e., temperature differences are the same in both scales.
  • Conversion between scales:
    • K=C+273.15K = C + 273.15
    • Where K is temperature in kelvin and C is temperature in Celsius.
  • Useful equivalent: 0 °C = 273.15 K; -273.15 °C corresponds to 0 K (absolute zero).

11.3 Practical Thermometers

  • Many physical properties vary with temperature, leading to different thermometer types that rely on different properties.
  • A thermocouple is a type of thermometer with a specific structure:
    • The reference junction is kept at a constant temperature, while the measurement junction is used to measure an unknown temperature.
    • If there is a temperature difference between the junctions, an emf is formed, which is measured by the voltmeter.
    • The temperature is calculated from the recorded emf using a calibration curve.
  • A thermistor is a semiconductor thermometer:
    • Its temperature decreases as its resistance increases (negative temperature coefficient).
    • The resistance can be measured and then converted to temperature using a calibration curve.
  • Both have advantages and disadvantages, summarized in the comparison below.

11.4 Thermocouple vs Thermistor: Feature Comparison

  • Feature: Sensitivity
    • Thermocouple: Sensitivity depends on the choice of metals in the two wires; can be made very sensitive.
    • Thermistor: Very sensitive but over a narrow temperature range.
  • Feature: Range
    • Thermocouple: Large temperature range.
    • Thermistor: Narrow temperature range.
  • Feature: Response time
    • Thermocouple: Junctions have small thermal capacity, so response time is short.
    • Thermistor: Larger thermal capacity, so response time is longer.
  • Feature: Stability
    • Thermocouple: Wires forming the junctions are subject to corrosion and aging effects may occur.
    • Thermistor: Very stable and mostly unaffected by aging.
  • Feature: Ease of use
    • Thermocouple: The reference junction must be kept at a constant temperature (often with ice water), which can be awkward; modern thermocouples have improved temperature compensation, making them easier to use.
    • Thermistor: Generally easier to use.
  • Note: An image in the original material shows the thermocouple structure with a reference junction and a measurement junction, and how emf arises from the temperature difference.