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UNIVERSIDAD CARLOS III DE MADRID UNIVERSIDAD CARLOS III DE MADRID Chemistry Chemistry TOPIC 2 1 Topic Topic 2. States States of of Matter Matter (I) (I) - Gases Gases. 1 States of Matter (I) - Gases

TOPIC 2 Statesof Matter(I) -Gases

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UNIVERSIDAD CARLOS III DE MADRIDUNIVERSIDAD CARLOS III DE MADRID

ChemistryChemistry

TOPIC 2

1TopicTopic 22.. StatesStates ofof MatterMatter (I)(I) -- GasesGases.. 1

States of Matter (I) - Gases

UNIVERSIDAD CARLOS III DE MADRIDUNIVERSIDAD CARLOS III DE MADRID

General Chemistry General Chemistry

Contents1. Introduction2. Pressure measurement3. The Ideal Gas equation4. Efusion and Diffusion

2TopicTopic 22.. StatesStates ofof MatterMatter (I)(I) -- GasesGases.. 2

4. Efusion and Diffusion5. Kinetic Molecular Theory6. Dalton’s Law of Partial Pressure7. Real Gases: van der Waals equation

UNIVERSIDAD CARLOS III DE MADRIDUNIVERSIDAD CARLOS III DE MADRID

General Chemistry General Chemistry

1. IntroductionStates of Matter

Distances Interactions Movement

3TopicTopic 22.. StatesStates ofof MatterMatter (I)(I) -- GasesGases.. 3

Solid Short Very strong Highly restricted

Liquids Short Strong Restricted

Gases Long Weak Almost Free

General Chemistry: Principles and Moderns ApplicationsR.H. Petrucci

UNIVERSIDAD CARLOS III DE MADRIDUNIVERSIDAD CARLOS III DE MADRID

General Chemistry General Chemistry

1. Introduction Where do we find gases?

4TopicTopic 22.. StatesStates ofof MatterMatter (I)(I) -- GasesGases.. 4

http://en.wikipedia.org/wiki/File:Michael_Schumacher_Ferrari_2004.jpg

http://en.wikipedia.org/wiki/File:Automobile_exhaust_gas.jpg

UNIVERSIDAD CARLOS III DE MADRIDUNIVERSIDAD CARLOS III DE MADRID

General Chemistry General Chemistry

2. Pressure Measurement

P = d·g·h

d = densityg = gravityh = height

Barometer

Column of

Vaccum

5TopicTopic 22.. StatesStates ofof MatterMatter (I)(I) -- GasesGases.. 5

h = height

1 atm = 760 mmHg ⇒⇒⇒⇒

atmospheric pressure at sea level

1 Torr = 1 mmHg

Pa = N/m2 <> 1/133.322 Torr

Standard Atmospheric Pressure 1.00 atm760 mm Hg, 760 Torr101.325 kPa1.01325 bar1013.25 mbar

Atmospheric pressure

Column of mercury

760 mmHg for standard atmosphere

UNIVERSIDAD CARLOS III DE MADRIDUNIVERSIDAD CARLOS III DE MADRID

General Chemistry General Chemistry

Manometer

2. Pressure Measurement

Closed end

Open end

Patm

6TopicTopic 22.. StatesStates ofof MatterMatter (I)(I) -- GasesGases.. 6

(a)

Pgas = Ph

Pgas

(b)

Pgas = Patm + Ph

Pgas

Ph = ρ(Hg)·g·h

ρ(Hg)= density of mercury13.6 g·cm3.

g = 9.8 m·s-2.h = distance B-N (in m).

UNIVERSIDAD CARLOS III DE MADRIDUNIVERSIDAD CARLOS III DE MADRID

General Chemistry General Chemistry

Boyle’s LawBoyle’s Law

3. Gases LawsP∝∝∝∝ 1/V when T & n are constant

P·V = k

7TopicTopic 22.. StatesStates ofof MatterMatter (I)(I) -- GasesGases.. 7

P·V = k

P1·V1 = P2·V2 = P3·V3 = · · · ·

For a fixed amount of an ideal gas at a constant temperature, pressure and volume areinversely proportional.

http://www.grc.nasa.gov/WWW/K-12/airplane/boyle.html

UNIVERSIDAD CARLOS III DE MADRIDUNIVERSIDAD CARLOS III DE MADRID

General Chemistry General Chemistry

3. Gases Laws

V ∝∝∝∝ T

V1/T1=V2/T2=k (P& n constant)

V = a(t + 273) where:

Charles and Gay-Lussac’s Law

8TopicTopic 22.. StatesStates ofof MatterMatter (I)(I) -- GasesGases.. 8

V = a(t + 273) where:

- V=volume

- t=temperature in Celsius

- a= slope of the straight line.

T = 273.15 + t

T=Absolute temperature (K)

Image from: http://www.unizar.es/lfnae/luzon/CDR3/charles.jpg

For a fixed amount of an ideal gas at a constant pressure, the volume is directlyproportional to the temperature. V = c· T

UNIVERSIDAD CARLOS III DE MADRIDUNIVERSIDAD CARLOS III DE MADRID

General Chemistry General Chemistry

TheThe Gas Gas ConstantConstant

• Boyle’s law V ∝ 1/P

• Charles’s law V ∝ T

• Avogadro’s law V ∝ n

nT

PV ∝ PV = nRTPV = nRT

The Ideal Gas equationThe Ideal Gas equation

3. Gases Laws

9TopicTopic 22.. StatesStates ofof MatterMatter (I)(I) -- GasesGases.. 9

TheThe Gas Gas ConstantConstant

R = 8,206�10-2 atm�l�mol-1�K-1

<> 8.314 J�mol-1�K-1 <> 1,987 cal�mol-1�K-1

At STP (0 ºC and 1atm) 1 mol gas = 22.4 L gas

Kmol

atmL

Kmol

Latm

nT

pVR 082.0

15.273*1

4.22*1 ===

UNIVERSIDAD CARLOS III DE MADRIDUNIVERSIDAD CARLOS III DE MADRID

General Chemistry General Chemistry

Diffusion

4. Diffusion and Efusion

10TopicTopic 22.. StatesStates ofof MatterMatter (I)(I) -- GasesGases.. 10

M

1R

1R

∝ρ

Graham’s Law

Graham's law states that the rate of diffusion of a certain gas isinversely proportional to the square root of its molecular weight.

UNIVERSIDAD CARLOS III DE MADRIDUNIVERSIDAD CARLOS III DE MADRID

General Chemistry General Chemistry

4. Diffusion and Efusion Why do tyres deflate?

Efusion

11TopicTopic 22.. StatesStates ofof MatterMatter (I)(I) -- GasesGases.. 11

A

B

B

A

M

M

R

R

B ofeffusion of rate

A ofeffusion of rate == Graham’s Law

UNIVERSIDAD CARLOS III DE MADRIDUNIVERSIDAD CARLOS III DE MADRID

General Chemistry General Chemistry

� Particles are point masses (with no volume) in constant,

random and straight line motion.

� Particles are separated by great distances, almost infinite.

� Collisions are elastic.

� There are no intermolecular forces between the particles.

5. Kinetic Molecular Theory Why do tyres deflate?

12TopicTopic 22.. StatesStates ofof MatterMatter (I)(I) -- GasesGases.. 12

� The total energy of the system remains constant.

V

NyProbabilit ∝

V

N=ion Concentrat

2umcollisionper Energy =

3liberty of Degrees =

V

uNmp

3

2

=

0 1000 2000 3000 4000 5000

No.

Mol

ecul

es (

%)

Speed (m/s)

um is the modal speed

uav is the simple average

urms2u=

umuav

urms

UNIVERSIDAD CARLOS III DE MADRIDUNIVERSIDAD CARLOS III DE MADRID

General Chemistry General Chemistry

5. Kinetic Molecular Theory

umN3

1PV 2

A=Let’s consider 1 mol of gas:

If PV = RT (for n= 1 mol):

Oxygen at 273 KM

3RTu rms =

Rel

ativ

e nu

mbe

r o

f M

olec

ules

(%)

13TopicTopic 22.. StatesStates ofof MatterMatter (I)(I) -- GasesGases.. 13

M

3RTu

uM3RT

umN3RT

rms

2

2

A

=

=

=

Considering that NAm = M:

0 1000 2000 3000 4000 5000

Hydrogen at 273 K

Oxygen at 1000 KR

elat

ive

num

ber

of

Mol

ecul

es (%

)

Speed (m/s)

UNIVERSIDAD CARLOS III DE MADRIDUNIVERSIDAD CARLOS III DE MADRID

General Chemistry General Chemistry

The total pressure of a mixture of gases is the sum of the pressures that each gas would

exert if it were present alone.

V , T constant∑=+++==

N

iiCBAT ppppp

1

···= Tii

where

pp χ:

6. Dalton’s Law of Partial Pressure

14TopicTopic 22.. StatesStates ofof MatterMatter (I)(I) -- GasesGases.. 14

P1 = 3.1 atm

P2 = 6.4 atmPtotal = P1 + P2 = 9.5 atm

V

RTnp ii =

pressure total

fraction mole

==

T

i

p

where

χ:

Example : Calculate the total pressure of a mixture of H2 and O2 whose partial pressures are PH2 =2.9 atm and PO2 = 7.2 atm respectively

UNIVERSIDAD CARLOS III DE MADRIDUNIVERSIDAD CARLOS III DE MADRID

General Chemistry General Chemistry

7. Real Gases

The factor “Z = PV/NRT” is known as COMPRESSIBILITY FACTOR and should be one for an ideal gas.

For exactly one mole of an ideal gas:

For exactly one mole of a real gas:

a) Effect of the nature of the gas b) Effect of the temperature

15TopicTopic 22.. StatesStates ofof MatterMatter (I)(I) -- GasesGases.. 15

0

1

2

0 200 400 600 800 1000 1200

NH3

CH4

H2

Ideal Gas

a) Effect of the nature of the gas b) Effect of the temperature

0

1

2

3

0 300 600 900

1000 K

500 K

200 K

Ideal Gas

0.1=RT

PV

P(atm)

0.1=RT

PV

P(atm)

UNIVERSIDAD CARLOS III DE MADRIDUNIVERSIDAD CARLOS III DE MADRID

General Chemistry General Chemistry

7. Real Gases

P + (V – nb) = nRTan2

V2( )

P · V = n·R·T The Ideal Gas Equation

The van der Waals Equation(a real gas equation)

16TopicTopic 22.. StatesStates ofof MatterMatter (I)(I) -- GasesGases.. 16

P + (V – nb) = nRTV2( )

PressureCorrection

VolumeCorrection

(a real gas equation)

a: Effect of intermolecular forces(i.e. nature of the gas)

b: Effect of molecular volume ���� Particles are NOT point masses (with no volume asstates the kinetic molecular theory).