Heat capacity (thermal capacity) is defined as the heat energy needed to raise the temperature of a whole body by one kelvin:
\[C = \frac{Q}{\Delta\theta}.\]
Its unit, \(\text{J K}^{-1}\), is itself a reminder of the definition: joules per kelvin of temperature change.
Convert the energy to joules before dividing, since the answer is wanted in \(\text{J K}^{-1}\):
\[Q = 48\ \text{kJ} = 48\,000\ \text{J}.\]
A temperature difference of \(53\ ^\circ\text{C}\) is the same size as a difference of \(53\ \text{K}\), because one Celsius degree and one kelvin represent the same interval; only the zero points of the two scales differ. There is therefore no need to add \(273\) to a temperature change. Substituting,
\[C = \frac{48\,000}{53} = 905.7\ \text{J K}^{-1}.\]
Two errors are worth guarding against. Adding \(273\) to the \(53\) gives \(326\ \text{K}\) and a much smaller capacity, and leaving the energy as \(48\ \text{kJ}\) gives \(0.906\), which is in \(\text{kJ K}^{-1}\) rather than the requested unit. Note also that this quantity applies to this particular body only; to obtain the specific heat capacity of the material you would additionally divide by the mass, using \(c = C/m\).