Thermal physics

Modes of heat transfer

Solids — particle to particleQ/t = kAΔT/L

Parameters

Hot temperature90 °C
Cold / surroundings temperature20 °C
Material

k = 385 W/mK

Cross-sectional area20 cm²
Rod length50 cm

Calculated

ΔT70 °C
Rate Q/t = kAΔT/L107.80 W
MaterialCopper
Directionhot → cold always

Curriculum

WAECNECOIGCSESATJUPEB

📋 Teacher notes

  • Particles do NOT travel down the rod — they vibrate in place and pass energy to their neighbours, like a row of people jiggling a rope.
  • Metals conduct well because free (delocalised) electrons carry energy quickly through the lattice; non-metals lack these free electrons.
  • Rate of heat flow: Q/t = kAΔT/L — bigger area or ΔT speeds it up, a thicker (longer) barrier slows it down. This is exactly why we use thick walls and small windows to keep buildings warm.
  • Compare copper (k≈385) with glass (k≈0.8): copper conducts about 480 times faster — try both in the material list.
  • Trapped air (double glazing, wool, fur) is a poor conductor and makes an excellent insulator, precisely because it has such a low k.

✏️ Exercises