Карточки Thermodynamic Processes | Quizlet

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26 Terms

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Isobaric

No change in pressure; Q = ΔU + W; W = nRΔT; W = PΔV

(Charles Law)

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Isochoric

No change in volume; W = 0; Q = ΔU

(Gay-Lussac's Law)

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Isothermal

No change in temperature; W = Q;

(Boyle's Law)

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Adiabatic

No heat added or removed; No change in entropy; ΔU = -W; ΔS = 0

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Entropy

The measure of disorder in a system; ΔS = ΔQ/T; Increases with Volume and Temperature

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Isothermal Compression

Gives off heat without changing internal temperature.

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Isothermal Expansion

Takes in heat without changing internal temperature.

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Isobaric Expansion

Work is positive and is found using pΔV or nRΔT.

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Isobaric Compression

Work is negative and is found using pΔV or nRΔT.

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Isochoric Expansion

Work is zero, Heat is positive, and Temperature increases.

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Isochoric Compression

Work is zero, Heat is negative, and Temperature decreases.

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Adiabatic Expansion

No change in heat; Temperature increases, while work(volume) decreases.

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Adiabatic Compression

No change in heat; Temperature decreases, while work(volume) increases.

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Work

A change in volume. Cannot occur without a change in volume. Can be found by finding the area under a Pressure-Volume graph.

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The First Law of Thermodynamics

Q = W + ΔU; Heat is equal to work plus change in internal temperature.

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The Second Law of Thermodynamics

For any cycle of energy, some heat must be lost.

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Work of a Heat Engine

Q(hot) - Q(cool) = Work; Q(hot) = Q(cool) + W

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Efficiency

The amount of heat that is converted to Work;

e = W/Q(hot); e = 1- Q(cool)/Q(hot)

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The Carnot Cycle

Theoretical cycle for the most efficient process of turning a given amount of heat into work.

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Efficiency of the Carnot Cycle

e(c) = 1 - T(cool)/T(hot); Temperature is in Kelvin.

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Isothermal Expansion

The first step of the Carnot Cycle. Constant hot temperature, takes in heat.

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Adiabatic Expansion

The second step of the Carnot Cycle. T(hot) becomes T(cool) with no change in heat.

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Isothermal Compression

The third step of the Carnot Cycle. Constant cold temperature, Heat leaves the engine.

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Adiabatic Compression

The last step of the Carnot Cycle. T(cool) becomes T(hot) with no change in heat.

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Temperature

The measure of average kinetic energy. Also indicates the direction of heat flow.

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Internal Energy

What heat becomes when absorbed by a gas.