1. How is temperature measured? T measurement is not based on a fundamental physical unit. Use a thermodynamic parameter (X) that varies in a known way with temperature. Measure its value at TWO fixed points of temperature and then interpolate and extrapolate. X Temp. FP 2 FP 1 X1X1 X2X2 Error! XmXm

2. n.b.p. = normal boiling point Ranges of various types of thermometer V P or V

3. Reference Points for Older Temperature Scales Daniel Fahrenheit (Danzig (Gdansk)1724) Anders Celsius (Sweden, 1742) Boiling point of water = 0 ºC ! Melting point of ice = 100 ºC! Values were later reversed. Scale called “centigrade” Ice, water and ammonium chloride mixture = 0 °F Human body = 96 °F (now taken as 98.6 °F) Two (or more) reference points result in errors when extrapolating outside of their range.

4. For 0 ºC < t < 850 ºC Pt Resistance Thermometer Blundell and Blundell, Concepts in Thermal Physics (2006)

5. Fixed temp. (cold junction) + - Unknown temp. (hot junction) V Seebeck effect Principle of Thermocouples

6. Reports on Progress in Physics, vol. 68 (2005) pp. 1043–1094 Metals used for Thermocouples Each type requires calibration against fixed points.

7. Radiation energy density Planck distribution law infrared UV-Vis. Spectral Distribution of Thermal Radiation

8. Stefan-Boltzmann equation: Thermal Radiation Compare radiation flux at an unknown temperature to the flux from a fixed point: triple point of water SB constant

9. Black Body Radiation from Au at its Melting Point Used to calibrate pyrometers. See presentation by Mark Owen at the Professional Training conference to hear about pyrometry at NPL.

10. Reports on Progress in Physics, vol. 68 (2005) pp. 1043–1094 Fixed Temperature Reference Points Melting points of metals and alloys

11. Defining a Temperature Scale with a Single Fixed Point X is a thermodynamic variable, T x is the temperature at which it is measured, and c is a constant. Requires a linear (monotonic) relationship: Also requires a single fixed point. There are several possibilities! By international agreement* in 1954, the so-called “thermodynamic temperature scale” uses the triple point (TP) of water defined - not measured! - to be 273.16 K. *Tenth General Conference on Weights and Measures

12. 0.006 The Triple Point of Water At the triple point of water: gas, solid and liquid all co- exist at a pressure of 0.006 atm.

13. Reports on Progress in Physics, vol. 68 (2005) pp. 1043–1094 Cell for Establishing the Triple Point of Water

14. Defining a Temperature Scale with a Single Fixed Point We see that: What thermodynamic variable should be measured to use the thermodynamic temperature scale? So,

15. The Gas Scale of Temperature Ideal gas law: TP = 273.16K Unknown T Gas P, V V and n are held constant.

16. A constant-volume gas thermometer

17. °C = K - 273.15 Relationship between °C and K: Defining the Kelvin and Celsius scales Note that careful measurements find that at 1 atm. water boils at 99.97 K above the melting point of ice (i.e. at 373.12 K). 1 K is not exactly equal to 1 °centigrade! “One Kelvin degree is 1/273.16 of the temperature of the triple point of water.” Named after William Thomson (Lord Kelvin) who was a professor at the University of Glasgow.

18. Proposed definition of the Kelvin Recognising that thermal energy is given by kT (where the Boltzmann constant is k = 1.38065 x 10 -23 JK -1 ), the Kelvin could be defined simply as: “The kelvin is the change of thermodynamic temperature that results in a change of thermal energy kT by 1.38065XX × 10 −23 Joule.” This definition requires a very precise measurement of k! Temperature scales have been refined as recently as 1990 (International Temperature Scale)

19. Reports on Progress in Physics, vol. 68 (2005) pp. 1043–1094 R = N A k

20. Measuring k with Brownian Motion x  is viscosity of fluid phase; r is the particle radius Random path Sub-  m polymer particles in water

21. Third Law of Thermodynamics Planck: The entropy of all systems is the same at 0K and may be taken to be zero. A temperature of 0 K is unattainable in a finite number of steps. Blundell and Blundell, Concepts in Thermal Physics (2006)