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PHY 231 1 PHYSICS 231 Lecture 26: Ideal gases Remco Zegers Walk-in hour: Thursday 11:30-13:30 am Helproom

PHYSICS 231 Lecture 26: Ideal gases

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PHYSICS 231 Lecture 26: Ideal gases. Remco Zegers Walk-in hour: Thursday 11:30-13:30 am Helproom. Ideal Gas: properties. Collection of atoms/molecules that Exert no force upon each other - PowerPoint PPT Presentation

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Page 1: PHYSICS 231 Lecture 26: Ideal gases

PHY 2311

PHYSICS 231Lecture 26: Ideal gases

Remco ZegersWalk-in hour: Thursday 11:30-13:30 am

Helproom

Page 2: PHYSICS 231 Lecture 26: Ideal gases

PHY 2312

Ideal Gas: properties

Collection of atoms/molecules that• Exert no force upon each other

The energy of a system of two atoms/molecules cannot be

reduced by bringing them close to each other• Take no volume

The volume taken by the atoms/molecules

is negligible compared to the volume they

are sitting in

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R

Potential Energy

0-Emin

Rmin

Ideal gas: we are neglecting the potential energy betweenThe atoms/molecules

R

Potential Energy

0

Kinetic energy

Page 4: PHYSICS 231 Lecture 26: Ideal gases

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Number of particles: mol

1 mol of particles: 6.02 x 1023 particlesAvogadro’s number NA=6.02x1023 particles per mol

It doesn’t matter what kind of particles:1 mol is always NA particles

Page 5: PHYSICS 231 Lecture 26: Ideal gases

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What is the weight of 1 mol of atoms?

X

Z

A

Number of protons

molar mass

Name

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Weight of 1 mol of atoms

1 mol of atoms: A gram (A: mass number)

Example: 1 mol of Carbon = 12 g 1 mol of Zinc = 65.4 g

What about molecules?H2O 1 mol of water molecules:

2x 1 g (due to Hydrogen)1x 16 g (due to Oxygen)

Total: 18 g

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Example

A cube of Silicon (molar mass 28.1 g) is 250 g.A) How much Silicon atoms are in the cube? B) What would be the mass for the same number of gold atoms (molar mass 197 g)

Page 8: PHYSICS 231 Lecture 26: Ideal gases

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Boyle’s Law

P0 V0 T0

2P0 ½V0 T0

½P0 2V0 T0

At constant temperature: P ~ 1/V

Page 9: PHYSICS 231 Lecture 26: Ideal gases

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Charles’ law

P0 V0 T0

P0 2V0 2T0

If you want to maintain a constant pressure, the temperature must be increased linearly with the volume V~T

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PHY 23110

Gay-Lussac’s law

P0 V0 T0 2P0 V0 2T0

If, at constant volume, the temperature is increased,the pressure will increase by the same factor

P ~ T

Page 11: PHYSICS 231 Lecture 26: Ideal gases

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Boyle & Charles & Gay-LussacIDEAL GAS LAW

PV/T = nR

n: number of particles in the gas (mol)R: universal gas constant 8.31 J/mol·K

If no molecules are extracted from or added to a system:

2

22

1

11 constant T

VP

T

VP

T

PV

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ExampleAn ideal gas occupies a volume of 1.0cm3 at 200C at1 atm. A) How many molecules are in the volume?B) If the pressure is reduced to 1.0x10-11 Pa, while thetemperature drops to 00C, how many molecules remainedin the volume?

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And another!An airbubble has a volume of 1.50 cm3at 950 m depth (T=7oC). What is its volume when it reaches the surface(water=1.0x103 kg/m3)?

Page 14: PHYSICS 231 Lecture 26: Ideal gases

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A small matter of definition

Ideal gas law: PV/T=nR PV/T=(N/NA)R

n (number of mols)=N (number of molecules)

NA (number of molecules in 1 mol)

Rewrite ideal gas law: PV/T = NkB

where kB=R/NA=1.38x10-23 J/K Boltzmann’s constant

Page 15: PHYSICS 231 Lecture 26: Ideal gases

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From macroscopic to microscopic descriptions: kinetic theory of gases

For derivations of the equations, see the textbook

1) The number of molecules is large (statistical model)2) Their average separation is large (take no volume)3) Molecules follow Newton’s laws4) Any particular molecule can move in any direction with a large distribution of velocities5) Molecules undergo elastic collision with each other6) Molecules make elastic collisions with the walls7) All molecules are of the same type

Page 16: PHYSICS 231 Lecture 26: Ideal gases

PHY 23116

Pressure

2

2

1

3

2vm

V

NP

Number of Molecules

Volume

Mass of 1 molecule

Averaged squared velocity

Average translation kinetic energy

Number of moleculesper unit volume

Page 17: PHYSICS 231 Lecture 26: Ideal gases

PHY 23117

M

RT

m

Tkvv

nRTTNkE

Tkvm

vmk

T

TNkPV

vmNPV

brms

Bkin

B

B

B

33

2

3

2

32

3

2

1

)2

1(

3

2

2

1

3

2

2

2

2

2

Microscopic

Macroscopic

Temperature ~ average molecular kinetic energy

Average molecular kinetic energy

Total kinetic energy

rms speed of a moleculeM=Molar mass (kg/mol)

Page 18: PHYSICS 231 Lecture 26: Ideal gases

PHY 23118

example

What is the rms speed of air at 1atm and room temperature? Assume it consist ofmolecular Nitrogen only (N2)?

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And another...

What is the total kinetic energy of the air molecules in thelecture room (assume only molecular nitrogen is present N2)?