For systems that simultaneously exhibit multiple irreversible transport processes, a result named for this function implies that the matrix of phenomenological coefficients is symmetric and positive-definite. (15[1])Those equations (15[1])named for this function are derived by Taylor expanding entropy in terms of a matrix L and won a Nobel prize for their discoverer, Lars Onsager. (15[2])For (15[1])a (15[1])system (-5[1])reversibly (15[2])exchanging (15[2])heat with its surroundings, (15[1])the integral of this function of temperature with respect to heat is the change (15[1])in (*) entropy, as in (-5[1])Clausius’s theorem. (10[2]-5[3])This function of the product (10[1])of Boltzmann’s (10[1])constant (-5[1])and temperature (10[1])yields (10[1])thermodynamic (10[1]-5[1])beta. (10[3]-5[3])This function (10[4])of pressure (10[1]-5[1])is proportional (10[2]-5[1])to (10[1])volume by Boyles’ law. (10[2]-5[3])For 10 points, (10[2]-5[1])“coldness” and temperature (0[1]-5[1])are related by what function, equivalent (-5[1])to an inverse (10[1]-5[1])proportion? (10[3])■END■ (10[14]0[7])