This experiment determines the specific latent heat of fusion of ice by supplying thermal energy electrically and observing the temperature change with time. During the phase change from solid to liquid, the supplied energy causes no temperature rise.
When heat is supplied to a substance undergoing a change of state, the temperature of the substance remains constant even though energy continues to be absorbed. This energy is known as latent heat.
The energy required to change the state of a mass \( m \) of a substance without changing its temperature is given by:
\[Q = mL\]
where \( L \) is the specific latent heat of fusion.
In this experiment, thermal energy is supplied electrically by an immersion heater. The electrical energy supplied is:
\[E = VIt\]
During the melting of ice at \(0^\circ\text{C}\), all the supplied energy is used to break intermolecular bonds, so:
\[VIt = mL\]
The latent heat of fusion can therefore be determined from the energy supplied during the constant-temperature region of the temperature–time graph.
A temperature–time graph shows an initial constant-temperature region at \(0^\circ\text{C}\) while the ice melts, followed by a rise in temperature once all the ice has turned into water.
For guidance on plotting graphs and identifying gradients and plateaus, visit our Graph Guide.
The temperature remains constant during the melting of ice despite continuous energy input. The specific latent heat of fusion of ice is determined from the energy supplied during this phase change.
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