Endothermic process

An endothermic process is any process with an increase in the enthalpy "H" (or internal energy "U") of the system. In such a process, a closed system usually absorbs thermal energy from its surroundings, which is heat transfer into the system. It may be a chemical process, such as dissolving ammonium nitrate in water, or a physical process, such as the melting of ice cubes. 
The term was coined by Marcellin Berthelot from the Greek roots "endo-", derived from the word "endon" (ἔνδον) meaning "within", and the root "therm" (θερμ-), meaning "hot" or "warm" in the sense that a process depends on absorbing heat if it is to proceed. The opposite of an endothermic process is an exothermic process, one that releases or "gives out" energy, usually in the form of heat and sometimes as electrical energy. Thus in each term (endothermic and exothermic) the prefix refers to where heat (or electrical energy) goes as the process occurs.
In chemistry.
Due to bonds breaking and forming during various processes (changes in state, chemical reactions), there is usually a change in energy. If the energy of the forming bonds is greater than the energy of the breaking bonds, then energy is released. This is known as an exothermic reaction. However, if more energy is needed to break the bonds than the energy being released, energy is taken up. Therefore, it is an endothermic reaction.
Details.
Whether a process can occur spontaneously depends not only on the enthalpy change but also on the entropy change (∆"S") and absolute temperature "T". If a process is a spontaneous process at a certain temperature, the products have a lower Gibbs free energy "G" = "H" - "TS" than the reactants (an exergonic process), even if the enthalpy of the products is higher. Thus, an endothermic process usually requires a favorable entropy increase (∆"S" > 0) in the system that overcomes the unfavorable increase in enthalpy so that still ∆"G" < 0. While endothermic phase transitions into more disordered states of higher entropy, e.g. melting and vaporization, are common, spontaneous chemical processes at moderate temperatures are rarely endothermic. The enthalpy increase ∆"H" » 0 in a hypothetical strongly endothermic process usually results in ∆"G" = ∆"H" -"T"∆"S" > 0, which means that the process will not occur (unless driven by electrical or photon energy). An example of an endothermic and exergonic process is
C6H12O6 + 6 H2O → 12 H2 + 6 CO2, ∆r"H°" = +627 kJ/mol, ∆r"G°" = -31 kJ/mol