Thermodynamics Ideal Mixtures
Tags: #physics #thermodynamics #ideal mixturesEquation
$$U_{\rm mixture}=\sum_i n_i U^0_i \\ H_{\rm mixture}=\sum_i n_i H^0_i \\ S_{\rm mixture}=n\sum_i x_i S^0_i+\Delta S_{\rm mix} \\ \Delta S_{\rm mix}=-nR\sum\limits_i x_i\ln(x_i)$$Latex Code
U_{\rm mixture}=\sum_i n_i U^0_i \\ H_{\rm mixture}=\sum_i n_i H^0_i \\ S_{\rm mixture}=n\sum_i x_i S^0_i+\Delta S_{\rm mix} \\ \Delta S_{\rm mix}=-nR\sum\limits_i x_i\ln(x_i)
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Introduction
Equation
Latex Code
U_{\rm mixture}=\sum_i n_i U^0_i \\ H_{\rm mixture}=\sum_i n_i H^0_i \\ S_{\rm mixture}=n\sum_i x_i S^0_i+\Delta S_{\rm mix} \\ \Delta S_{\rm mix}=-nR\sum\limits_i x_i\ln(x_i)
Explanation
Latex code for the Ideal Mixtures. I will briefly introduce the notations in this formulation.
: one component in a second gives rise to an increase in the boiling point
: one component in a second gives rise to decrease of the freezing point
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