Giant mechanocaloric materials for solid-state cooling |
(a) and (b) Absolute value for the isothermal entropy change and adiabatic temperature change, respectively, as a function of the applied uniaxial stress for selected elastocaloric materials. (c) and (d) Absolute value of isothermal entropy change and adiabatic temperature change, respectively, as a function of the hydrostatic pressure for selected barocaloric materials. |