1 lec 5: thermodynamic properties, pvt behavior. 2 for next time: –read: § 3-5 –hw 3 due sept...

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1 Lec 5: Thermodynamic properties, Pvt behavior

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Page 1: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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Lec 5: Thermodynamic properties, Pvt behavior

Page 2: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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• For next time:– Read: § 3-5– HW 3 due Sept 17

• Outline:– Buoyancy and stability– Pure substances and processes– Property diagrams for pure substances

• Important points:– How to calculate point of action of hydrostatic load– The general shape of the property diagrams– How to solve problems using the property diagrams

Page 3: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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Properties - Introduction

• We have discussed extensive properties such as U, m, and V (for volume) which depend on the size or extent of a system, and

• Intensive properties such as u, v, T, and P which are independent of system extent (engineers are ambivalent about nomenclature for pressure, sometimes using p and P interchangeably)

Page 4: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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Important questions...

• How many properties are needed to define the state of a system?

• How do we obtain those properties?

Page 5: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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For a simple system,

• We may write: p = p(v,T)

• or perhaps: v = v(p,T).

Page 6: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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Pure

• Pure means “…of uniform and invariable chemical composition (but more than one molecular type is allowed).” This allows a single phase of air to be a pure substance.

• All our substances will be pure. We will drop the use of the word. When we refer to a simple system we mean one filled with a pure substance--a simple, pure system.

Page 7: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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For a simple, pure substance

• y1 = f(y2,y3), or

• p = p(v,T), v = v(p,T) and T = T(p,v)

• What do these equations define, in space?

• Equations used to relate properties are called “equations of state”

Page 8: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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Ideal gas “law” is a simple equation of state

RTPvM

RR u

Ru = universal gas constant

m = mass

n = number of moles

M = molar mass or molecular weight

mRTPV TnRPV u

Page 9: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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Behavior of real substances

• Lets consider substances that do not obey the perfect gas law– certainly not as a solid– certainly not as a liquid– sometimes not very well as a gas

Page 10: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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Phase Change Process of a Pure Substance

P=1 atmT=20°C

P=1 atmT=100°C

P=1 atmT=100°C

P=1 atmT=250°C

P=1 atmT=100°C

liquid liquid liq/vap

vapor vapor

Page 11: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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Consider a constant pressure process (of water)

Page 12: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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T-v Diagram

Page 13: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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Page 14: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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You should be able to discuss characteristics of the following:

• Liquid to liquid/vapor to vapor transition (begin with a constant pressure process).

• Single phase regions--liquid, vapor, solid.• Two-phase regions--liquid/vapor and

solid/vapor.• Melting--solid to liquid (freezing)• vaporization--liquid to vapor (liquefaction)• sublimation--solid to vapor

Page 15: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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Page 16: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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Notice the triple-state line. Along this line all

three states exist in equilibrium

For water, the triple point is at 273.16 K (32.018 F) and 0.6113 kPa (0.0887 psia).

Page 17: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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Vapor Dome - region encompassing the two-phase, vapor-liquid equilibrium region

Saturated vapor line

Saturated liquid line

Page 18: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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Critical Point

• Point at which the saturated vapor and saturated liquid lines coincide.

• If T Tc or P Pc there is no clear distinction between the superheated vapor region and the compressed liquid region.

• Substances in this region are sometimes known as “fluids” rather than as vapors or liquids.

• By convention, if P Pc, and T Tc we refer to the fluid as superheated. If P Pc, and T < Tc we refer to the fluid as a subcooled or compressed liquid.

Page 19: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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Phase Diagram (PT-coordinates)

P

T

Solid PhaseRegion

LiquidPhaseRegion

Superheated G asPhase Region

M eltingCurve

T rip leState

CriticalState

Page 20: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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GAS @ gGAS

State d

W eight

LIQUID

GAS

W eight

LIQUID @ a

P

T

g

P

T

g

d

P

T

g

d

a

Superheated Vapor

Compressed Liquid

Constant Temperature Process

Q

Page 21: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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P

T

b

Gas @ bGas @ b

Q

GAS

STATE f

LIQUID

Q

GASLIQUID

Q

P

T

bf

P

T

bfa

Superheated Vapor

Subcooled Liquid

Constant Pressure Process

Page 22: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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Page 23: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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P

v

Superheated Region

Saturation Region

Subcooled Region

Critical Point

Sat. Vapor Line

Sat. Liquid Line

Page 24: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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Page 25: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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Saturation temperature

• Temperature at which a phase change takes place at a given pressure.

Page 26: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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Saturation pressure

• Pressure at which a phase change takes place at a given temperature.

Page 27: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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TEAMPLAYTEAMPLAY

• Discuss what happens when water boils on the stove at your residence. Start with a pan of water at 70 F, 1 atm pressure.

QContinued on next slide.

Page 28: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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TEAMPLAY (CONTINUED)TEAMPLAY (CONTINUED)• What is the pressure at various times

during the entire process?

• Does the temperature of the water change?

• If the vapor (steam) were contained in an elastic container, what would happen as heat continued to be added after all the liquid disappeared.

• Sketch pV and TV diagrams.

Page 29: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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Saturation properties

• Along the saturated liquid line, properties are identified by the subscript “f”

• Along the saturated vapor line, properties are identified by the subscript “g”

•Both sets of properties can be found in the temperature and pressure tables in your book’s appendices.

•Both tables give the same data.

•There are different tables for different substances.

Page 30: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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Temperature table (also known as a saturation table)

Table A-4

Page 31: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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Pressure table (also known as a saturation table)

Table A-5

Page 32: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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[Two properties are not independent in the vapor dome

(the two-phase region)]

• The temperature and pressure are uniquely related. Knowing a T defines the P and vice versa.

Page 33: 1 Lec 5: Thermodynamic properties, Pvt behavior. 2 For next time: –Read: § 3-5 –HW 3 due Sept 17 Outline: –Buoyancy and stability –Pure substances and

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TEAMPLAYTEAMPLAY

• Find, for Refrigerant 134a, the following properties: the saturation pressure at a saturation temperature of -10 F.

• and find for the same substance the saturation temperature at a pressure of 0.06 MPa.

• Make sure everyone in your group understands how to do this.