thermodynamics continues. volume expansion Δv = βv 0 Δt where β is the coefficient of volume...

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Thermodynamics Continues

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Page 1: Thermodynamics Continues. Volume Expansion ΔV = βV 0 ΔT where β is the coefficient of volume expansion Example: 4 liters of gasoline is heated from 2

Thermodynamics Continues

Page 2: Thermodynamics Continues. Volume Expansion ΔV = βV 0 ΔT where β is the coefficient of volume expansion Example: 4 liters of gasoline is heated from 2

Volume Expansion

ΔV = βV0 ΔT where β is the coefficient of volume expansion

Example: 4 liters of gasoline is heated from 20 C to 870C. How much is the volume of the gasoline increased?

Ans: 3.23 x10-4m3 or 323 L

Page 3: Thermodynamics Continues. Volume Expansion ΔV = βV 0 ΔT where β is the coefficient of volume expansion Example: 4 liters of gasoline is heated from 2

Water isn’t the only weird one!!! What does water have in common with Lead,

Uranium, Neon and Silicon? They all expand when they freeze. Other

elements contract. Water is at it’s highest density at 40C. Due to its hydrogen and crystal structure as it

freezes, ice is less dense than water.

Page 4: Thermodynamics Continues. Volume Expansion ΔV = βV 0 ΔT where β is the coefficient of volume expansion Example: 4 liters of gasoline is heated from 2

Boyle’s Law

Volume of a gas is inversely proportional to the pressure applied when kept at constant temperature.

V is proportional to 1/p

V1P1 = V2P2

Page 5: Thermodynamics Continues. Volume Expansion ΔV = βV 0 ΔT where β is the coefficient of volume expansion Example: 4 liters of gasoline is heated from 2

Charles Law

Volume of a gas is directly proportional the Temperature when kept at constant pressure.

V is proportional to T

V1 /T1 = V2 /T2

Page 6: Thermodynamics Continues. Volume Expansion ΔV = βV 0 ΔT where β is the coefficient of volume expansion Example: 4 liters of gasoline is heated from 2

Guy-Lussac’s Law

Pressure is proportional to Temperature when kept at constant Volume

P proportional to T at constant V

P1 / T1 = P2 / T2

Page 7: Thermodynamics Continues. Volume Expansion ΔV = βV 0 ΔT where β is the coefficient of volume expansion Example: 4 liters of gasoline is heated from 2

Ideal Gas Law PV = nRT

P Pressure Pa or N/m2 atm V Volume m3 L n moles mol mol R Universal Gas Constant

J/mol K L atm/mol K T Temperature K K

1 Pa = 1N/m2 1 atm = 1.013x105 Pa = 101.3 kPa

R = 8.315 J/mol K = .0821 L atm/mol K

Moles # of grams = to molecular mass

Page 8: Thermodynamics Continues. Volume Expansion ΔV = βV 0 ΔT where β is the coefficient of volume expansion Example: 4 liters of gasoline is heated from 2

STP

Standard Temperature and Pressure T = 273 K P = 1 atm = 101.3 kPa Example: What is the volume of one mole of

gas at STP? Ans: 22.4 L

Page 9: Thermodynamics Continues. Volume Expansion ΔV = βV 0 ΔT where β is the coefficient of volume expansion Example: 4 liters of gasoline is heated from 2

Looking further ….

PV/T = nR = constant !!! P1V1 = P2V2

T1 T2

Page 10: Thermodynamics Continues. Volume Expansion ΔV = βV 0 ΔT where β is the coefficient of volume expansion Example: 4 liters of gasoline is heated from 2

Try a problem

Example: A tire has 200 kPa of pressure at 100C. IF the tire heats to 400C, what is the pressure of the tire? (Hint assume no change in volume.)

Ans: 221 kPa

Page 11: Thermodynamics Continues. Volume Expansion ΔV = βV 0 ΔT where β is the coefficient of volume expansion Example: 4 liters of gasoline is heated from 2

Avagadro’s # and Boltzman’s Constant Avagadro’s number – NA = 6.02x1023

molecules per mole PV = NkT

Where N = number of molecules K = Boltzman’s Constant 1.38x10-23J/K = R/NA

Page 12: Thermodynamics Continues. Volume Expansion ΔV = βV 0 ΔT where β is the coefficient of volume expansion Example: 4 liters of gasoline is heated from 2

Kinetic Theory of Gases

Connection between what happens on the microscopic level and what we observed on the macroscopic level.

Imagine a gas made of a collection of molecules moving inside a container of volume V….

Page 13: Thermodynamics Continues. Volume Expansion ΔV = βV 0 ΔT where β is the coefficient of volume expansion Example: 4 liters of gasoline is heated from 2

Assumptions - Kinetic Theory of Gases Container holds a large #, N, of identical

molecules, each with a mass m and which behaves as a point particle;

Molecules move randomly in the container, obeying Newton’s Laws of motion at all times;

When molecules hit the walls or other molecules they behave in a perfectly elastic manner.

Page 14: Thermodynamics Continues. Volume Expansion ΔV = βV 0 ΔT where β is the coefficient of volume expansion Example: 4 liters of gasoline is heated from 2

Pressure Relationship

Due to the assumptions, pressure of a gas can be related to the behavior of the molecules themselves.

Page 15: Thermodynamics Continues. Volume Expansion ΔV = βV 0 ΔT where β is the coefficient of volume expansion Example: 4 liters of gasoline is heated from 2

Kinetic Theory

KEavg = ½ mvavg2 = (3/2) kT

Solve for v vrms = √(v2)avg

vrms = (√3kT/m)

Page 16: Thermodynamics Continues. Volume Expansion ΔV = βV 0 ΔT where β is the coefficient of volume expansion Example: 4 liters of gasoline is heated from 2

Kinetic Energy and Temperature ½ mv2 = KEavg= 3 /2 kT

Page 17: Thermodynamics Continues. Volume Expansion ΔV = βV 0 ΔT where β is the coefficient of volume expansion Example: 4 liters of gasoline is heated from 2

HEAT

Calorie – Heat needed to raise 1 g of water 10C Kilocalorie (Calorie) Heat needed to raise 1 kg

of water 10 C English Unit: BTU 1 kcal = 4186 J – Mechanical Equivalent of Heat Heat: Energy transferred from one thing to

another due to a difference in temperature.

Page 18: Thermodynamics Continues. Volume Expansion ΔV = βV 0 ΔT where β is the coefficient of volume expansion Example: 4 liters of gasoline is heated from 2

Heat vs. Thermal Energy

Heat: Energy Transfer

Thermal Energy: Internal Energy

U = 3/2 nRT U = Internal Energy

Q = mcΔT Q = Heat c = Specific Heat

Qlost= Q gained so… m1c1(Tf – T1)+ m2c2(Tf – T1) =0

or… m1c1(Tf – T1) = m2c2(T1 – Tf)

Page 19: Thermodynamics Continues. Volume Expansion ΔV = βV 0 ΔT where β is the coefficient of volume expansion Example: 4 liters of gasoline is heated from 2

Change of Phase

Heat of Fusion: Heat needed to take something from a solid to a liquid

Heat of Vaporization: Heat needed to take something from a liquid to a gas

Latent Heat (L): Heat values for heat of fusion or heat of vaporization

Q = mL m = mass L = latent heat

Page 20: Thermodynamics Continues. Volume Expansion ΔV = βV 0 ΔT where β is the coefficient of volume expansion Example: 4 liters of gasoline is heated from 2

Research and Present (Separately): 1st Law of Thermodynamics: Daniel

2nd Law of Thermodynamics: Molly Heat Death: Sarah Entropy: Megan, Andrew L. Carnot Cycle: Andy K. Heat Engines: Chris, Christine Heat Pumps and Refrigerators: Derek Conduction (Include R-value): Elizabeth, Tim Radiation and the Stefan-Boltzman Equation, Max

5 min max, Can discuss (don’t have to) with other person to avoid presenting duplication but each must research work individually and present individually. Due ______