CONTENTS. xi PAGE $4.Equivalence Values of the Transformations. 07 $5.Combined value of all the Transformations which take place in a single Cyclical Process 101 6.Proof that in a reversible Cyclical Process the total value of all the Transformations must be equal to nothing 102 7.On the Temperatures of the various quantities of Heat;and the Entropy of the body 10G n the Function of Temperature,r.. 107 CHAPTER V. FORMATION OF THE TWO FUNDAMENTAL EQUATIONS. $1.Discussion of the Variables which determine the Condition of the body. 110 $2.Elimination of the quantities U and S from the two fundamental equations 112 3.Case in which the Temperature is taken as one of the Independent Variables 115 84. Particular Assumptions as to the External Forces 116 85. Frequently occurring forms of the differential equations 118 $6.Equations in the case of a body which undergoes a partial change 87. Clapeyron'Equation and Camota Funetion in its condition of aggregation 119 CHAPTER VI. APPLICATION OF THE MECHANICAL THEORY OF HEAT TO SATURATED VAPOUR. $1.Fundamental equations for Saturated Vapour 126 s2. Specific Heat of Saturated Steam 129 83. Numerical Value of h for Steam 133 84. Numerical Value of h for other vapours 135 85. Specifio Heat of Saturated Steam as proved by experiment. 189 86. Specifio Volume of Saturated Vapour 142 7..Departure from the law of Mariotte and Gay-Lussao in the case of Saturated Steam .143 8.Differential-coeficienta of pa .148 D8n $9.A Formula to determine the Specific volume of Saturated Steam, and its comparison with Experiment 150 $10.Determination of the Mechanical Equivalent of Heat from the behaviour of Saturated Steam,·· 155 时Google§ 4. § 5. § 6. § 7. § 8. § 1. § 2. § 3. §4. § 5. § 6. § 7. CONTENTS. xi PAGB Equivalence Values of the Transformations. • • • • 97 Combined value of all the Transformations which take place in a single Cyclical Process. • • • • • • 101 Proof that in a reversible Cyclical Process the total value of all the Transformations must be equal to nothing • • • 102 On the Temperatures of the various quantities of Heat; and the Entropy of the body • • 106 On the Function of Temperature, T 107 CHAPTER V. FORHATION OF THE TWO FUlfDAMENTAL EQUATIONS. Discussion of the Variables which determine the Condition of the body • • • • • . • • • • . 110 EIimination of the quantities U and 8 from the two fundamental equations • • • • • • • . • . 112 Case in which the Temperature is taken as one of the Independent Variables • • • • • • •• 115 Particular Assumptions as to the External Forces .' 116 Frequently occurring forms of the differential equations • • 118 Equations in the ease of a body which undergoe8 a partial change in its condition of aggregation • • 119 Clapeyron's Equation and Carnot's Function 121 CHAPTER VI. APPLICATION OF THE MECHANICAL THEORY OF HEAT TO SATURATED VAPOUR. § 1. Fundamental equstions for Saturated Vapour 126 § 2. Specific Heat of Saturated Steam 129 § 3. Numerical Value of h for Steam. . 133 § 4. Numerical Value of h for other vapours . • .. 135 § 5. Specific Heat of Saturated Steam as proved by experiment. 139 § 6. Specific Volume of Saturated Vapour. . • . . • 142 § 7. • Departure from the law of Mariotte and Gay-LussaCl in the case of Saturated Steam 143 § 8. Differential-coefficients of ~ 148 PIn § 9. A Formula to determine the Specific volume of Saturated Steam, and its comparison with Experiment • • • • • 150 § 10. Determination of the Mechanical Equivalent of Heat from the behaviour of Saturated Steam. 155 Digitized by Coogle