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Name Chapter 16 Class Date Thermal Energy and Heat Section 16.2 Heat and Thermodynamics (pages 479483) This section discusses three kinds of thermal energy transfer and introduces the first, second,.
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Thermodynamics FAQ
The second law of thermodynamics can be expressed as the following: It is impossible in any system for heat transfer from a reservoir to completely convert to work in a cyclical process in which the system returns to its initial state.
Thus, by the first law of thermodynamics, the work done for each complete cycle must be W = Q1 − Q2. In other words, the work done for each complete cycle is just the difference between the heat Q1 absorbed by the engine at a high temperature and the heat Q2 exhausted at a lower temperature.
The Second Law of Thermodynamics (first expression) Heat transfer occurs spontaneously from higher- to lower-temperature bodies but never spontaneously in the reverse direction. Another way of stating this: It is impossible for any process to have as its sole result heat transfer from a cooler to a hotter object.
A fundamental rule that determines the fate of the universe. The second law of thermodynamics means hot things always cool unless you do something to stop them. It expresses a fundamental and simple truth about the universe: that disorder, characterised as a quantity known as entropy, always … increases.
The first law of thermodynamics states that the change in internal energy of a system equals the net heat transfer into the system minus the net work done by the system. In equation form, the first law of thermodynamics is ΔU = Q − W. Here ΔU is the change in internal energy U of the system.
The second law of thermodynamics requires that heat is transferred from one body to another body only if the two bodies are at different temperatures, and that the heat flows from the body at the highest temperature to the body at the lowest temperature.
The first-law equation ΔU=q+w sets up a balance sheet for the energy of the system, measured in the local frame, by equating its change during a process to the net quantity of energy transferred by means of heat and work.
Essentially, this law states that heat does not naturally flow from a cool body to a warmer; work must be expended to make it do so.
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