Chapter 3: Thermodynamics Flashcards

1
Q

temperature conversions

A

F = 9/5 C + 32

K = C + 273

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2
Q

thermal expansion equation

A

ΔL =αLΔT

ΔL = change in lenght
α = coefficient of linear expansion
L = original lenght
ΔT = change in temperature

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3
Q

volume expansion equation

A

ΔV = βVΔT

ΔV = change in volume
β = coefficient of volumetric expansion
L = original volume
ΔT = change in temperature

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4
Q

First law of thermodynamics

A

ΔU = Q - W

ΔU = change in internal energy
Q = energy tranfered into the system
W = work done by the system

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5
Q

heat gained or lost (with temperature change)

A

q = m c ΔT

c = specific heat of the substance
m = mass in Kg

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6
Q

heat gained or lost (phase change)

A

q = mL

m = mass
q = heat
L = heat of tranformation or letent heat

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7
Q

entropy and heat

A

ΔS = Qrev / T

ΔS = change in entropy
Qrev = heat gained or lost in a reversible processs
T = temperature in K

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8
Q

second law of thermodynamics

A

ΔSuniverse = ΔSsystem + ΔSsurrounding > 0

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9
Q

isothermal ΔU =0

A

Q = W

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9
Q

adiabatic (Q = 0)

A

ΔU = - W

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9
Q

isovolumetric or isochoric ( W = 0)

A

ΔU = Q

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10
Q

work equations for a cylinder with contant preure and change nin volume

A

W = P ΔV

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11
Q

0 degrees celsius

A

272 K

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12
Q

100 degree C

A

373 K

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13
Q

Zeroth law of thermodynamics.

A

When one objects in thermal equilibrium with another object and the second objects in thermal equilibrium with the third object, then the 1st and 3rd object are also in thermic equilibrium.

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14
Q

Temperature

A

Differences in temperature determine the direction of heat transfer. Temperatures proportional to the average kinetic energy of a particle that makes up the substance. Heat moves spontaneously from materials that have higher temperature to materials that have lower temperature.

15
Q

Heat

A

refers to the transfer of thermal energy from hotter objects with higher temperature to a colder object with lower temperature. If no net heat flows between the objects in thermal contact, then we can say that their temperatures are equal and that they are in thermal equilibrium.

15
Q

Kelvin scale.

A

It defines as the zero reference point absolute 0, the theoretical temperature at which there is no thermal energy and sets the freezing point of water as 273K.

15
Q

Third law of thermodynamics.

A

States that the entropy of a perfectly organized crystal are absolute 00.

16
Q

Body temperature.

A

98.6 Fahrenheit or 37 Celsius.

17
Q

Thermal Expansion.

A

Rising temperatures cause an increase in length and falling temperatures cause a decrease in length. The amount of length changes the proportional to the origin length of the solid and the increasing temperature.

18
Q

Coefficient of linear expansion α

A

Constant that characterized how a specific material’s length changes.

18
Q

Coefficient of volumetric expansion β

A

Constant the characterizes how a specific materials volume changes as the temperature changes.

19
Q

Relationship between coefficient of volumetric expansion and coefficient of linear expansion.

A

Β = 3α

20
Q

Isolated systems.

A

Not capable of exchanging energy or matter with the surroundings. An example is a bomb calorimeter.

21
Q

Closed system.

A

Capable of exchanging energy but not matter with the surrounding.

22
Q

State functions.

A

Independent of the path taken to get to a particular equilibrium state. Some examples are pressure density, temperature, volume, enthalpy, internal energy, Gibbs free energy, entropy.

22
Q

Open system.

A

Can exchange both matter and energy with the environment.

23
Q

First law of thermodynamics.

A

States that the change in the total internal energy of a system is equal to the amount of energy transferred in the form of heat to the system minus the amount of energy transferred from the system in the form of work. The internal energy of a system can be increased by adding heat, doing work on the system, or some combination of both. Internal energy of a system will decrease when heat is lost from the system where work is performed by the system.

24
Q

Second law of thermodynamics.

A

Objects in thermal contact and not in thermal equilibrium will exchange heat energy such that the object with the higher temperature will give off the heat energy to the object with lower temperature until both objects have the same temperature at thermal equilibrium.

25
Q

Conduction.

A

The direct transfer of energy from molecule to molecule through molecular collision. There must be direct physical contact. Metals are described as the best heat conductors because metallic bonds contain a density of atoms embedded in a sea of electrons.

26
Q

Convection.

A

The transfer of heat by the physical motion of a fluid over a material. Only liquids and gases can transfer heat by this mean.

27
Q

Conversion factors between the units of heat.

A

1 Cal = 10^3 cal = 4184 J = 3.97 BTU

27
Q

Radiation.

A

Is a transfer of energy by electromagnetic waves.

28
Q

What is the specific heat of water?

A

1 cal/g.K

29
Q

Special types of thermodynamic processes.

A

Isothermal, which has constant temperature and therefore no change in internal energy, adiabatic, which has no heat exchange, and isovolumetric no change in volume and therefore no work accomplished.

30
Q

Entropy

A

Measure of the spontaneous dispersal of energy at a specific temperature. How much energy is spread out, or how widely spread out energy becomes in a process. The units of entropy are usually J/mol.K

31
Q

Natural processes and irreversibility.

A

When a hot object is brought into thermal contact with a cold object, the object will transfer heat in the energy to the code object until both are intermolecular Librium. This is a natural process and is also one that it would be described as irreversible. We are not surprised that the two objects eventually would reach a common temperature, but. You would be shocked if all of a sudden the hot object became hotter and the cold object became colder. This would be an unnatural process.