chap3a jan13

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CHAPTER 3a CHAPTER 3a PROPERTIES OF PURE SUBSTANCES PROPERTIES OF PURE SUBSTANCES

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Page 1: Chap3a jan13

CHAPTER 3aCHAPTER 3a

PROPERTIES OF PURE SUBSTANCES

PROPERTIES OF PURE SUBSTANCES

Page 2: Chap3a jan13

CONTENTSCONTENTS

Pure Subtances

Phases of a Pure Substances

Phase Change Processes

Property Diagrams

Property Tables

The Ideal Gas Equation

Compressibility Factor

Page 3: Chap3a jan13

Define a pure substance

Explain the phase change processes

Sketch P-v and T-v diagrams for a particular process

At the end of the lesson, you should be able to:

LESSON OBJECTIVESLESSON OBJECTIVES

Page 4: Chap3a jan13

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PURE SUBSTANCEPURE SUBSTANCE

Pure substance: A substance that has a fixed chemical composition throughout.

Air is a mixture of several gases, but it is considered to be a pure substance.

Nitrogen and gaseous air are pure substances.

A mixture of liquid and gaseous water is a pure substance, but a mixture of liquid and gaseous air is not.

Page 5: Chap3a jan13

PHASES OF A PURE SUBSTANCEPHASES OF A PURE SUBSTANCE

The molecules in a solid are kept at their positions by the large springlike inter-molecular forces.

In a solid, the attractive and repulsive forces between the molecules tend to maintain them at relatively constant distances from each other.

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Page 7: Chap3a jan13

PHASE-CHANGE PROCESSES OF PURE SUBSTANCES

PHASE-CHANGE PROCESSES OF PURE SUBSTANCES

At 1 atm and 20°C, water exists in the liquid phase (compressed liquid: not about to vaporize).

At 1 atm pressure and 100°C, water exists as a liquid that is ready to vaporize (saturated liquid: about to vaporize).

Let us consider the following system undergoes heating process at constant pressure.

As more heat is transferred, part of the saturated liquid vaporizes (saturated liquid–vapor mixture: liquid and vapor coexist in equilibrium).

At 1 atm pressure, the temperature remains constant at 100°C until the last drop of liquid is vaporized (saturated vapor: about to condense).

As more heat is transferred, the temperature of the vapor starts to rise (superheated vapor: not about to condense).

Page 8: Chap3a jan13

T-v diagram for the heating process of water at constant pressure.

PHASE-CHANGE PROCESSES OF PURE SUBSTANCES (cont’d)

PHASE-CHANGE PROCESSES OF PURE SUBSTANCES (cont’d)

The constant pressure heating process (state 1 - 5) can be illustrated in the following figure known as the T-v Diagram

Saturation state: State at which a phase change begins or ends

Page 9: Chap3a jan13

Consider repeating this process for other constant pressure lines as shown below. (Where are the saturated liquid and vapour line?)

Critical point: The point at which the saturated liquid and saturated vapor states are identical.

Page 10: Chap3a jan13

SATURATION TEMPERATURE AND SATURATION PRESSURESATURATION TEMPERATURE AND SATURATION PRESSURE

The temperature at which water starts boiling depends on the pressure; therefore, if the pressure is fixed, so is the boiling temperature.

Water boils at 100C at 1 atm pressure.

Saturation temperature Tsat: The temperature at which a pure substance changes phase at a given pressure.

Saturation pressure Psat: The pressure at which a pure substance changes phase at a given temperature.

Page 11: Chap3a jan13

Where are the saturation temperatures for P1 and P2?

PROPERTY DIAGRAMS:

T-v Diagram of Pure Substance

PROPERTY DIAGRAMS:

T-v Diagram of Pure Substance

Page 12: Chap3a jan13

Where are the saturation pressures for T1 and T2 ?

PROPERTY DIAGRAMS:

P-v Diagram of Pure Substance

PROPERTY DIAGRAMS:

P-v Diagram of Pure Substance

Page 13: Chap3a jan13

Sketch T-v and P-v diagram for the following processes, withrespect to saturation lines. Show initial and final states.

1. A piston cylinder device contains (by mass) 50% liquid water and50% water vapour in equilibrium at 800 kPa (Tsat=170.4°C). Heatis transferred at constant pressure until temperature reaches350°C.

2. Superheated water vapour at 15 bar, T=400°C is allowed to coolat constant volume until it becomes saturated water vapour.

3. A piston cylinder device contains compressed liquid water. Heat isadded to the system at constant pressure until the entire liquidis vaporized.

EXERCISESEXERCISES

Page 14: Chap3a jan13

Extending the Diagrams to Include The Solid Phase

Extending the Diagrams to Include The Solid Phase

P-v diagram of a substance that contracts on freezing.

P-v diagram of a substance that expands on freezing (such as water).

Triple line: All 3 phases of a pure substance coexist in equilibrium (substance have same P & T but different v)

Page 15: Chap3a jan13

Sublimation:: Passing from the solid phase directly into the vapor phase.

At low pressures (below the triple-point value), solids evaporate without melting first (sublimation).

P-T diagram of pure substances.

At triple-point pressure and temperature, a substance exists in three phases in equilibrium.

For water, Ttp = 0.01°C

Ptp = 0.6117 kPa

PHASE DIAGRAMPHASE DIAGRAM

Page 16: Chap3a jan13

P-v-T surface of a substance that contracts on freezing.

P-v-T surface of a substance that expands on freezing (like water).

The P-v-T surfaces present a great deal of information at once, but in a thermodynamic analysis it is more convenient to work with two-dimensional diagrams, such as the P-v and T-v diagrams.

PVT SURFACEPVT SURFACE

Page 17: Chap3a jan13

Class TakeawayClass Takeaway

Indicate the following states of a pure substance on P-v and T-vdiagrams:

(a) Saturated liquid line

(b) Saturated vapour line

(c) Critical point

(d) Triple point line

(e) Saturation temperature lines at 1 and 10 bar

(f) Constant pressure lines at 100oC and 200oC