The heat capacity of a material is a measure of the heat energy (in J) that the material (of mass M in g or moles) absorbs or releases for every unit rise or fall in temperature (in °C or K).

Whilst the heat capacity of most materials will generally be different at different temperatures and pressures, as they undergo internal structural changes with temperature, the heat capacity is generally quoted at a given temperature and pressure. These are typically quoted as 'standard conditions' (as defined by the various standard authorities around the world). For example, the National Institute of Standards and Technology (NIST) defines 'standard conditions' as 20°C and 1atm.
Now, copper is a solid below the temperature of 1358 K (1085°C) and has a specific heat capacity of 0.386 J/g.K or 24.5 J/mol.K (at 20°C and 1 atm).
Various empirical formulae exist which allow one to calculate the specific heat capacity of copper at other temperatures, based on measurements taken in various experiments and fitting the data to various curves such as cubic splines.
Refer to http://www.nist.gov/data/PDFfiles/jpcrd263.pdf for more information.
Copper is a liquid between the temperature of 1358K and 2835 K (2562°C) with true specific heat capacity of 0.572 J/g/K or 36.33 J/mol.K at a temperature of 1400K.
More accurate values of specific heat are given by suitable curve-fitting formulae, based on experimental data. (See: http://link.springer.com/article/10.1007%2FBF02755998)
Above it's boiling point of 2835 K (2562°C) copper vapourises. Copper gas has specific heat capacity of 25.14 (at 3000K) or at other temperatures, given by the Shomate Equation: $c_p(t)=A+Bt+Ct^2+Dt^3+Et^{-2}$
where
$t$ is the temperature in Kelvin / 1000
$A = -80.48635$
$B= 49.35865$
$C=-7.578061$
$D=0.404960$
$E=133.3382$
Source: http://webbook.nist.gov/cgi/cbook.cgi?ID=C7440508&Type=JANAFG&Table=on#JANAFG
References:
http://www.nist.gov/data/PDFfiles/jpcrd263.pdf