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Chapter 12 Properties Of Gases.

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Presentation on theme: "Chapter 12 Properties Of Gases."— Presentation transcript:

1 Chapter 12 Properties Of Gases

2 Pressure Measure of the number of collisions between gas particles and a unit area of the wall of the container Pressure = force / unit area

3 Force/area English system: pounds/in2 (psi) Metric system:
Newton/m2 (pascal)

4 Torricelli Barometer h = 760 mm Hg 1 atmosphere pressure

5 1 atm = 760 torr (mm Hg) = kPa = bar =14.70 psi

6

7 Patm Manometer h Pgas

8 Patm Manometer h Pgas

9 Volume Total space of a container that gases occupy due to the free random motion of the gas molecules

10 Relationship between Volume & Pressure of Gases
P-V

11 V P (at constant T)

12 Slope = k V 1/P (at constant T)

13 In mathematical terms:
y = mx + b Boyle’s Law

14 Relationship between Volume & Temperature of Gases
V-T

15 In mathematical terms:
y = mx + b V = mT + b Charles’ Law

16 Where T must be in Kelvin (K) temperature
K = 0C + 273

17

18 Relationship between Pressure & Temperature of Gases
P-T

19 In mathematical terms:
y = mx + b P = mT + b Gay-Lussac’s Law

20 Relationship between Volume & Moles
of Gases V-n

21 In mathematical terms:
y = mx + b V = mn + b Avogadro’s Law

22 Avogadro’s Hypothesis
At constant temperature and pressure, equal volumes of gases contain equal number of particles

23 Combined Gas Law

24 Ideal & Real Gasses

25 Kinetic Molecular Theory
1. Gases consist of small particles that are far apart in comparison to their own size. These particles are considered to be tiny points occupying a negligible volume compared to that of their container.

26 Kinetic Molecular Theory
2. Molecules are in rapid and random straight-line motion. This motion can be described by well-defined and established laws of motion.

27 Kinetic Molecular Theory
3. The collisions of molecules with the walls of a container or with other molecules are perfectly elastic. That is, no loss of energy occurs.

28 Kinetic Molecular Theory
4. There are no attractive forces between molecules or between molecules and the walls with which they collide.

29 Kinetic Molecular Theory
5. At any particular instant, the molecules in a given sample of gas do not all possess the same amount of energy.

30 Ideal Gas Equation

31

32 Note that is similar to the Combined Gas Law derived earlier.

33 Variations on Ideal Gas Equation

34 Variations on Ideal Gas Equation
Bromine Variations on Ideal Gas Equation

35 Real Gas Behavior

36 Ideal Gas Equation P V = n R T

37 N2 2.0 CH4 H2 PV nRT 1.0 Ideal gas CO2 P (atm)

38 “correct” for volume of molecules
(V - b)

39 attractive forces between molecules
also “correct” for attractive forces between molecules

40 van der Waals’ Equation
for 1 mole

41 van der Waals’ Equation
for n moles

42 from CRC Handbook a* b* He Ne *when P(atm) & V(L)

43 from CRC Handbook a* b* NH H2O *when P(atm) & V(L)

44 from CRC Handbook a* b* CCl C5H *when P(atm) & V(L)

45 Cl2 gas has a = 6.49, b = For 8.0 mol Cl2 in a 4.0 L tank at 27oC. P (ideal) = nRT/V = 49.3 atm P (van der Waals) = 29.5 atm

46 T & P conditions where a real gas approximates an ideal gas?

47 N2 gas PV nRT 203 K 293 K 1.8 1.4 673 K Ideal 1.0 gas 0.6
P (atm)

48 T & P conditions where a real gas approximates an ideal gas? high temperature low pressure

49 Gaseous Molecular Movement

50 pressure exerted by each component in a mixture of gases
Partial Pressure pressure exerted by each component in a mixture of gases

51 this assumes that NO interactions occurs between the molecules of gas

52 must conclude 1. each gas acts as if it is in container alone
2. each gas collides with the container wall as an “event”

53 where n = # components Or Dalton’s Law PT = P1 + P2 + P

54 Pi V = ni R T or

55 thus:

56 or

57 therefore: nT =  ni and PT  sum of mols of gas

58 Mole Fraction

59

60 Since: and

61 Then

62 and Pi = Xi PT

63

64 diffusion is the gradual mixing of molecules of different gases.
effusion is the movement of molecules through a small hole into an empty container.

65 rate of  average effusion speed

66

67 But ... where

68 thus then RMS speed

69

70

71 substituting:

72 simplifying Graham’s Law NH3-HCl

73

74 if “d” is constant

75 if “t” is constant

76 GAS LAW STOICHIOMETRY


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