CAIE A-Level Physics 14.3.2 Specific Latent Heat
Practise defining specific latent heat, distinguishing fusion from vaporisation and using delta Q = ml for constant-temperature phase changes.
- Syllabus
- 2028–2030
- Course
- Physics 9702
- Level
- A2
Practise defining specific latent heat, distinguishing fusion from vaporisation and using delta Q = ml for constant-temperature phase changes.
State what is meant by specific latent heat.
(thermal) energy per unit mass (to change state)
B1
change of state without any change of temperature
B1
A student uses the apparatus illustrated in Fig. 3.1 to determine a value for the specific latent heat of fusion of ice.

Fig. 3.1
The balance reading measures the mass of the beaker and the melted ice (water) in the beaker.
The heater is switched on and pieces of ice at 0∘C are added continuously to the funnel so that the heater is always surrounded by ice.
When water drips out of the funnel at a constant rate, the balance reading is noted at 2.0 minute intervals. After 10 minutes, the current in the heater is increased and the balance readings are taken for a further 12 minutes.
The variation with time of the balance reading is shown in Fig. 3.2.

Fig. 3.2
The readings of the ammeter and of the voltmeter are shown in Fig. 3.3.

Fig. 3.3
Determine a value for the specific latent heat of fusion L of ice.
VIt =m L
C1
({15.1×3.6}+R)×600=140×L or ({7.3×1.8}+R)×600=65×L
C1
41.22×600=75×L
C1
L=330 J g−1
A1
Calculate the rate at which thermal energy is transferred from the surroundings to the ice.
rate = W
15.1×3.6×600=(140×330)−H or 7.3×1.8×600=(65×330)−H
C1
H=13600
rate of gain = 13600/ 600
= 23 W
A1