《热的解析理论》(Theorie Analytique de la Chaleur)是法国著名数学家、物理学家 Joseph Fourier (1768 &ndash
- 目录
- 前辅文
- Preliminary Discourse
- CHAPTER I.Introduction.
- SECTION I.Statement of the Object of the Work.
- ART.
- 1. Object of the theoretical researches
- 12. First statement of the problem of the terrestrial temperatures.
- 13—15. Conditions necessary to applications of the theory. Object of the experiments.
- SECTION II.Preliminary Definitions and General Notions.
- 22—24. Permanent temperature, thermometer. The temperature denoted by 0 is that of melting ice. The temperature of water boiling in a given vessel under a given pressure is denoted by 1.
- 25. The unit which serves to measure quantities of heat, is the heat required to liquify a certain mass of ice
- 26. Specific capacity for heat
- 30. Notion of external conducibility.
- 31. We may at first regard the quantity of heat lost as proportional to the temperature. This proposition is not sensibly true except for certain limits of temperature.
- 32—35. The heat lost into the medium consists of several parts. The effect is compound and variable. Luminous heat
- 36. Measure of the external conducibility.
- 37. Notion of the conducibility proper. This property also may be observed in liquids
- 38, 39. Equilibrium of temperatures. The effect is independent of contact
- 50, 51. First notion of the effects of reflected heat
- 52—56. Remarks on the statical or dynamical properties of heat. It is the principle of elasticity. The elastic force of aeriform fluids exactly indicates their temperatures.
- SECTION III.Principle of the Communication of Heat.
- SECTION IV.On the Uniform and Linear Movement of Heat.
- 66, 67. Notion and measure of the flow of heat
- 68, 69. Measure of the conducibility proper.
- 70. Remarks on the case in which the direct action of the heat extends to a sensible distance
- 71. State of the same solid when the upper plane is exposed to the air
- 72. General conditions of the linear movement of heat.
- SECTION V.Law of the Permanent Temperatures in a Prism of Small Thickness.
- 73—80. Equation of the linear movement of heat in the prism. Different consequences of this equation
- SECTION VI.On the Heating of Closed Spaces.