To experimentally determine the entropy of a substance at standard state, one begins with the Third Law of Thermodynamics, which states that the entropy of a pure crystalline substance is zero at absolute zero. The entropy change can be calculated using the formula ΔS = ∫(dQ_rev/T). To find the entropy at standard state, this integral must be evaluated along a path from absolute zero to the standard state, often by heating at constant pressure. The resulting expression for entropy involves the heat capacity at constant pressure, S = ∫(c_P dT/T), which necessitates measuring the heat capacity as a function of temperature. A significant challenge arises in accurately measuring the heat capacity near absolute zero. To address this, researchers typically measure the heat capacity as closely as possible to absolute zero and apply the Debye approximation to refine their estimates of heat capacity in that region.