The flat part of the curve
Heat a pot of ice and watch the thermometer. It climbs to 0 °C, then STOPS while the ice melts, then climbs again to 100 °C, then stops again while the water boils. Those flat stretches are not the kettle resting. They are the most expensive parts of the whole journey.
— Q equals m L. is the heat in kilojoules, is the mass changing phase in kilograms, and is the specific latent heat in kJ/kg: what one kilogram costs to change phase, at constant temperature. Latent means hidden — hidden from the thermometer, because the energy goes into pulling molecules apart rather than into making them jiggle faster. There is no in this relation, and that absence is the entire point.
Water carries two of them, and mixing them up is the named mistake of this lesson. , the latent heat of fusion, is 334 kJ/kg: melting ice, or freezing water. , the latent heat of vaporisation, is 2257 kJ/kg at atmospheric pressure: boiling water, or condensing steam. The subscripts name the phase change, not an order of events.
Put those beside sensible heat and the scale of it lands. Melting a kilogram of ice costs about the same as warming that kilogram of water by eighty degrees. Boiling it costs nearly seven times more again. A steam plant is built the way it is because of that second number: steam carries a colossal amount of energy per kilogram, and hands every joule of it back the moment it condenses on something cold.