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IGCSE · Year 10–11SPM · Form 4Physics Standard

Specific Heat Capacity: Why the Time Must Be in Seconds

By Adrian Wong · 21 October 2026

The question

A student wants to measure the specific heat capacity of aluminium. She places a 50 W50\ \text{W} electric heater and a thermometer into holes in an aluminium block of mass 0.75 kg0.75\ \text{kg}. The block is wrapped in insulation.

The starting temperature of the block is 19.5∘C19.5^\circ\text{C}. She switches on the heater for 6.06.0 minutes, and the highest temperature reached by the block is 44.5∘C44.5^\circ\text{C}.

(a) Calculate the energy supplied by the heater. [2 marks]

(b) Assuming all of this energy goes into the block, calculate the specific heat capacity of aluminium. [3 marks]

(c) A data book gives the specific heat capacity of aluminium as 900 J/(kg ∘C)900\ \text{J/(kg}\ {}^\circ\text{C)}. Suggest why the student’s value is higher. [1 mark]

Cambridge IGCSE note: the equation for specific heat capacity is Extended content in 0625.

The common wrong answer

Most students start well. They remember E=PtE = Pt and put in the numbers from the question:

E=50×6.0=300 JE = 50 \times 6.0 = 300\ \text{J}

Then they find the temperature change correctly, 44.5−19.5=25.0∘C44.5 - 19.5 = 25.0^\circ\text{C}, and use c=EmΔθc = \dfrac{E}{m\Delta\theta}:

c=3000.75×25.0=16 J/(kg ∘C)c = \frac{300}{0.75 \times 25.0} = 16\ \text{J/(kg}\ {}^\circ\text{C)}

The mistake is in the very first line. A watt is a joule per second, so E=PtE = Pt only gives joules when tt is in seconds. Using 6.06.0 minutes makes the energy, and so the specific heat capacity, exactly 60 times too small. A value of 16 J/(kg ∘C)16\ \text{J/(kg}\ {}^\circ\text{C)} would mean aluminium heats up about 260 times more easily than water, which should ring alarm bells.

A second slip I often see is using the final temperature, 44.5∘C44.5^\circ\text{C}, instead of the temperature change. That gives about 539 J/(kg ∘C)539\ \text{J/(kg}\ {}^\circ\text{C)}, which is also wrong.

The correct working

(a) Convert the time to seconds first:

t=6.0×60=360 st = 6.0 \times 60 = 360\ \text{s} E=Pt=50×360=18 000 JE = Pt = 50 \times 360 = 18\,000\ \text{J}

The energy supplied is 18 000 J18\,000\ \text{J} (18 kJ18\ \text{kJ}).

(b) Temperature change:

Δθ=44.5−19.5=25.0∘C\Delta\theta = 44.5 - 19.5 = 25.0^\circ\text{C}

Rearrange E=mcΔθE = mc\Delta\theta for cc:

c=EmΔθ=18 0000.75×25.0=18 00018.75=960c = \frac{E}{m\Delta\theta} = \frac{18\,000}{0.75 \times 25.0} = \frac{18\,000}{18.75} = 960

The specific heat capacity is 960 J/(kg ∘C)960\ \text{J/(kg}\ {}^\circ\text{C)}.

(c) Some of the energy from the heater is lost to the surroundings (and some heats the heater and thermometer), so less than 18 000 J18\,000\ \text{J} actually goes into the block. Using the full 18 000 J18\,000\ \text{J} in the calculation makes cc come out too high.

Why it works

Power is the rate of transferring energy: 50 W50\ \text{W} means 5050 joules every second. To find the total energy you multiply by the number of seconds. In 6.06.0 minutes there are 360360 of them, so the heater gives out 18 000 J18\,000\ \text{J}, not 300 J300\ \text{J}.

Specific heat capacity is the energy needed to raise the temperature of 1 kg1\ \text{kg} by 1∘C1^\circ\text{C}. That’s why the equation uses the change in temperature: the block didn’t warm up from 0∘C0^\circ\text{C}, so the starting temperature has to come off.

For part (c), it helps to see the numbers. With the data-book value, warming this block by 25.0∘C25.0^\circ\text{C} needs 0.75×900×25.0=16 875 J0.75 \times 900 \times 25.0 = 16\,875\ \text{J}. The heater supplied 18 000 J18\,000\ \text{J}, so about 1 125 J1\,125\ \text{J} went somewhere other than the block. Insulation reduces that loss but never removes it, which is why this experiment almost always gives a value that is a little too high.

How to spot it next time

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