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Thermal Physics Kinetic Molecular Theory of Matter

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Kinetic Molecular Theory of Matter. Thermal Physics. Heat. The process by which energy is exchanged between objects because of temperature differences is called heat Objects are in thermal contact if energy can be exchanged between them - PowerPoint PPT Presentation

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Page 1: Kinetic Molecular Theory of Matter

Thermal Physics

Kinetic Molecular Theory of Matter

Page 2: Kinetic Molecular Theory of Matter

Heat

The process by which energy is exchanged between objects because of temperature differences is called heat

Objects are in thermal contact if energy can be exchanged between them

Thermal equilibrium exists when two objects in thermal contact with each other cease to exchange energy

Page 3: Kinetic Molecular Theory of Matter

Zeroth Law of Thermodynamics

If objects A and B are separately in thermal equilibrium with a third object, C, then A and B are in thermal equilibrium with each other.

Allows a definition of temperature

Page 4: Kinetic Molecular Theory of Matter

Temperature from the Zeroth Law

Two objects in thermal equilibrium with each other are at the same temperature

Temperature is the property that determines whether or not an object is in thermal equilibrium with other objects

Page 5: Kinetic Molecular Theory of Matter

Thermometers

Used to measure the temperature of an object or a systemMake use of physical properties that change with temperatureMany physical properties can be used• volume of a liquid

• length of a solid

• pressure of a gas held at constant volume

• volume of a gas held at constant pressure

• electric resistance of a conductor

• color of a very hot object

Page 6: Kinetic Molecular Theory of Matter

Thermometers, cont

A mercury thermometer is an example of a common thermometerThe level of the mercury rises due to thermal expansionTemperature can be defined by the height of the mercury column

Page 7: Kinetic Molecular Theory of Matter

Temperature Scales

Thermometers can be calibrated by placing them in thermal contact with an environment that remains at constant temperature

• Environment could be mixture of ice and water in thermal equilibrium

• Also commonly used is water and steam in thermal equilibrium

Page 8: Kinetic Molecular Theory of Matter

Celsius Scale

Temperature of an ice-water mixture is defined as 0º C

• This is the freezing point of water

Temperature of a water-steam mixture is defined as 100º C

• This is the boiling point of water

Distance between these points is divided into 100 segments or degrees

Page 9: Kinetic Molecular Theory of Matter

Gas Thermometer

Temperature readings are nearly independent of the gasPressure varies with temperature when maintaining a constant volume

Page 10: Kinetic Molecular Theory of Matter

Kelvin Scale

When the pressure of a gas goes to zero, its temperature is –273.15º C

This temperature is called absolute zero

This is the zero point of the Kelvin scale

• –273.15º C = 0 K

To convert: TC = TK – 273.15

• The size of the degree in the Kelvin scale is the same as the size of a Celsius degree

Page 11: Kinetic Molecular Theory of Matter

Pressure-Temperature Graph

All gases extrapolate to the same temperature at zero pressure

This temperature is absolute zero

Page 12: Kinetic Molecular Theory of Matter

Modern Definition of Kelvin Scale

Defined in terms of two points

• Agreed upon by International Committee on Weights and Measures in 1954

First point is absolute zero

Second point is the triple point of water

• Triple point is the single point where water can exist as solid, liquid, and gas

• Single temperature and pressure

• Occurs at 0.01º C and P = 4.58 mm Hg

Page 13: Kinetic Molecular Theory of Matter

Modern Definition of Kelvin Scale

The temperature of the triple point on the Kelvin scale is 273.16 K

Therefore, the current definition of of the Kelvin is defined as

1/273.16 of the temperature of the triple point of water

Page 14: Kinetic Molecular Theory of Matter

Some representative Kelvin temperatures

Note, this scale is logarithmic

Absolute zero has never been reached

Page 15: Kinetic Molecular Theory of Matter

Fahrenheit Scales

Most common scale used in the US

Temperature of the freezing point is 32º

Temperature of the boiling point is 212º

180 divisions between the points

Page 16: Kinetic Molecular Theory of Matter

Comparing Temperature Scales

Page 17: Kinetic Molecular Theory of Matter

Temperature Scales

273.15

932

55

329

95

C K

F C

C F

F C

T T

T T

T T

T T

Page 18: Kinetic Molecular Theory of Matter

Ideal Gas

A gas does not have a fixed volume or pressure

In a container, the gas expands to fill the container

Most gases at room temperature and pressure behave approximately as an ideal gas

Page 19: Kinetic Molecular Theory of Matter

Characteristics of an Ideal Gas

Collection of atoms or molecules that move randomly

Exert no long-range force on one another

Each particle is individually point-like

• Occupying a negligible volume

Page 20: Kinetic Molecular Theory of Matter

Moles

It’s convenient to express the amount of gas in a given volume in terms of the number of moles, n

One mole is the amount of the substance that contains as many particles as there are atoms in 12 g of carbon-12

massmolar

massn

Page 21: Kinetic Molecular Theory of Matter

Avogadro’s Number

The number of particles in a mole is called Avogadro’s Number

• NA=6.02 x 1023 particles / mole

• Defined so that 12 g of carbon contains NA atoms

The mass of an individual atom can be calculated:

Aatom N

massmolarm

Page 22: Kinetic Molecular Theory of Matter

Avogadro’s Number and Masses

The mass in grams of one Avogadro's number of an element is numerically the same as the mass of one atom of the element, expressed in atomic mass units, u

Carbon has a mass of 12 u

• 12 g of carbon consists of NA atoms of carbon

Holds for molecules, also

Page 23: Kinetic Molecular Theory of Matter

Your Turn

Find the mass (in kg) of a single atom of Argon.

Page 24: Kinetic Molecular Theory of Matter

Ideal Gas Law

PV = n R T

• R is the Universal Gas Constant

• R = 8.31 J / mole.K

• R = 0.0821 L. atm / mole.K

• Is the equation of state for an ideal gas

• This gas law was determined empirically.

Page 25: Kinetic Molecular Theory of Matter

Problem: An Expanding Gas

An ideal gas at 20o C and a pressure of 1.5 x 105 Pa is in a container having a volume of 1 L.

• (a) Determine the number of moles of gas in the container.

• (b) The gas pushes against a piston, expanding to twice its original volume, while the pressure falls to atmospheric pressure. Find the final temperature.

Page 26: Kinetic Molecular Theory of Matter

Problem: An Expanding Gas

(a) Find the number of gas moles.

• Convert the temperature to Kelvin:

• Solve the ideal gas law for n and substitute:

K 29327320273TT C

nRTPV

mol106.16.K)(293K)(8.31J/mol

)m10Pa)(110(1.5

RT

PVn 2

335

Page 27: Kinetic Molecular Theory of Matter

Problem: An Expanding Gas

Find the temperature after the gas expands to 2 L.

• Divide the ideal gas law for the final state by the ideal gas law for the initial state:

i

f

ii

ff

nRT

nRT

VP

VP

(293K)Pa)(1L)10(1.5

Pa)(2L)10(1.01T

VP

VPT

5

5

iii

fff

395KTf

Page 28: Kinetic Molecular Theory of Matter

Ideal Gas Law, Physics Version

P V = N kB T

• kB is Boltzmann’s Constant

• kB = R / NA = 1.38 x 10-23 J/ K

• N is the total number of molecules

n = N / NA

• n is the number of moles

• N is the number of molecules

Page 29: Kinetic Molecular Theory of Matter

Kinetic Theory of Gases

The number of molecules in the gas is large and the average separation between them is large compared to their dimensions

The molecules obey Newton’s laws of motion, but as a whole they move randomly

Page 30: Kinetic Molecular Theory of Matter

Kinetic Theory of Gases

The molecules interact only by short-range forces during elastic collisionsThe molecules make elastic collisions with the wallsThe gas under consideration is a pure substance, all the molecules are identical

Page 31: Kinetic Molecular Theory of Matter

Visualizing an Ideal Gas

http://www.phy.ntnu.edu.tw/ntnujava/index.php?topic=25

Page 32: Kinetic Molecular Theory of Matter

Ideal Gas Law, Derivation

Using our physics knowledge, we can now derive the ideal gas law from first principles.

Page 33: Kinetic Molecular Theory of Matter

Pressure of an Ideal Gas

The pressure is proportional to the number of molecules per unit volume and to the average translational kinetic energy of a molecule

2mv

2

1

V

N

2

3P

Page 34: Kinetic Molecular Theory of Matter

Pressure, cont

The pressure is proportional to the number of molecules per unit volume and to the average translational kinetic energy of the moleculePressure can be increased by

• Increasing the number of molecules per unit volume in the container

• Increasing the average translational kinetic energy of the molecules• Increasing the temperature of the gas

Page 35: Kinetic Molecular Theory of Matter

Molecular Interpretation of Temperature

Temperature is proportional to the average kinetic energy of the molecules

The total kinetic energy is proportional to the absolute temperature

Tk2

3mv

2

1B

2

nRT2

3KEtotal

Page 36: Kinetic Molecular Theory of Matter

Internal Energy

In a monatomic gas, the KE is the only type of energy the molecules can have

U is the internal energy of the gasIn a polyatomic gas, additional possibilities for contributions to the internal energy are rotational and vibrational energy in the molecules

nRT2

3U

Page 37: Kinetic Molecular Theory of Matter

Speed of the Molecules

Expressed as the root-mean-square (rms) speed

At a given temperature, lighter molecules move faster, on average, than heavier ones

• Lighter molecules can more easily reach escape speed from the earth

M

TR3

m

Tk3v B

rms

Page 38: Kinetic Molecular Theory of Matter

Some rms Speeds