Lesson 1 (Properties of Pure Substance)

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    Thermodynamics 2 Lesson 1

    LESSON 1

    PROPERTIES OF PURE SUBSTANCE

    DEFINITIONS AND USEFUL INFORMATION

    Pure substance is a substance that is homogeneous in composition and homogeneous and invariable in

    chemical aggregation (Faires, 1978).

    A substance is said to be pure substance if its chemical compositions do not change even in solid,

    liquid, or gaseous phase. Example of which is water that has two atoms of hydrogen and one atom of

    oxygen as it is in solid, liquid or gaseous state.

    State of pure substance or system refers to its condition as quantified or identified through the

    thermodynamic properties of the substance.

    Phase is a quantity of substance that is homogeneous throughout.

    Relevant Reversible Work Modes refers only to the important work modes for the system in question

    and irreversible work modes are not considered.

    Reversible work mode refers to the amount of energy added in a forward process that can be removed

    by the reversed process.

    Additional Thermodynamic Properties1. Enthalpy is a thermodynamic property with the following definitions:

    For a closed system, it means the sum of internal energy and the product of pressure andspecific volume, and given by the relation:

    pvuh +=

    Where, h = enthalpy, kJ/kg, Btu/lb p = pressure, kPaa, psia

    v = specific volume, m3/kg

    For an open system, enthalpy means the sum of internal energy and the flow energy or flowwork, and given by the relation:

    fEUH +=

    Where, H = total enthalpy, kJ, kW, Btu, Btu/min

    U = total internal energy, kJ, kW, Btu, Btu/min

    Ef= flow energy or work, kJ. KW, Btu, Btu/min

    2. Entropy is a thermodynamic property first introduced by Clausius in 1865 and could be defined asfollows:

    Entropy is the measure of the microscopic disorder of the molecules of a substance.

    It is a thermodynamic property that remains constant in an adiabatic reversible process. The change of entropy in an irreversible process is the measure of the unavailable energy. Entropy is also defined as the measure of the irreversibility of the system or substance. The change of entropy for a reversible process is given by the relation:

    ==

    rev

    12T

    dQsss

    Details of entropy werre discussed in the Second law of thermodynamics.

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    Thermodynamics 2 Lesson 1

    Explanation for the Change of Phase in Figure 1.1o At state 1, water is at solid phase at, say, - 20 C under atmospheric pressure of 101.325 kPa. Heat

    is added to the solid water to undergo the process from state 1 to state 2 without melting. This

    process is heating of solid with temperature increases from 20oC to 0

    oC.

    o At state 2, water is still at solid phase at 0 oC. This is the time in which melting process is about tostart. With the heat addition continues, melting process is from state 2 to state 3. During the

    melting process, temperature remains the same at 0

    o

    C. The temperature for process 2 to 3 isknown as melting temperature or melting point.

    o State 3 is the end of melting process but the temperature remains 0 oC. Water at this point is atliquid phase. Then heat addition continues to perform heating process from state 3 to state 4.

    During this process, temperature increases to, say, 60 oC.

    o At state 4, water is called subcooled liquid and the temperature is called subcooled liquidtemperature. Water heated but still no occurring of evaporation. With the heat addition continues,

    process 4 to 5 is performed with the increase of temperature from 60 oC to 100 oC. This process is

    still heating process.

    o At state 5, water is called as saturated liquid and at this point evaporation or boiling process isabout to start at 100 oC. With the heat addition continues, process 5 to 6 is performed without

    changing the temperature.

    o At state 6, water is a mixture liquid and vapor and is called as wet vapor or wet steam. At his pointthe temperature remains the same at 100

    oC. The proportion of the liquid and vapor components

    depends on time being considered from state 5 to state 6. The amount of vapor content may bedetermined if the quality of vapor or steam is given. With the heat addition continues, evaporation

    process is performed from state 6 to state 7 with the same temperature at 100 oC.

    o At state 7, boiling or evaporation process ended with the temperature still 100 oC. At this point, allliquid are converted into vapor or steam and is called as saturated vapor/steam or dry and saturated

    vapor/steam. With the heat addition continues, process 7 to 8 is performed with an increase of

    temperature from 100oC to, say, 150

    oC.

    Temperature for processes 5 to 6 and 6 to 7 is called boiling temperature or boiling point andtechnically termed in thermodynamics as saturation temperature and the existing pressure is

    also called as saturation pressure.

    o At state 8, the condition of water is called superheated vapor/steam and the temperature issuperheated vapor temperature at, say, 150 oC. The temperature at this point is higher than the

    saturation temperature. Any point above point 7 at a given temperature higher than the saturation

    temperature and following the same existing pressure is called as superheated vapor or steam. The difference of superheated temperature and the saturation temperature or boiling

    temperature is called degrees of superheat(oSH).

    The difference of saturation temperature and the subcolled liquid temperature is calleddegrees subcooled(

    oSC).

    Note:

    If the existing pressure is increased, melting and boiling temperatures are also increased. Withfurther increased of an existing pressure, a critical point is attained, a point in which saturated

    liquid and saturated vapor conditions are coexisted in equilibrium.

    If the existing pressure is decreased, melting and boiling temperatures are also decreased. With thefurther decreased of an existing pressure, a triple point will be attained, a point in which melting

    and boiling temperatures are the same. Existing pressure lower than the triple point, sublimation

    will take place.

    OTHER DEFINITIONS Existing pressure or applied pressure refers to the pressure of the system in which change of phase at

    constant pressure is considered.

    Solid water is a condition of water in which the temperature is below the freezing temperature

    corresponding to an existing pressure.

    Subcooled liquid is a liquid condition in which the given temperature is higher than the melting

    temperature and lower than the saturation or boiling temperature corresponding to an existing pressure.

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    Thermodynamics 2 Lesson 1

    Compressed liquid is a liquid condition in which the pressure is higher than saturation pressure

    corresponding to the given temperature.

    Saturated liquid is a liquid condition in which boiling or evaporation is about to begin and with the

    temperature is equal to the saturation or boiling temperature corresponding to an existing pressure.

    Wet vapor or wet steam is the mixture of saturated liquid and saturated vapor with the temperature

    equal to the saturation temperature corresponding to an existing pressure.

    Saturated vapor/steam or dry and saturated vapor/steam is vapor condition in which evaporation is

    ended and condensation is about to begin with the temperature equal to the saturation temperature

    equal to the saturation temperature corresponding to an existing pressures.

    Superheated vapor or steam is a vapor in which the temperature is higher than the saturation

    temperature corresponding to an existing pressure.

    Heat of fusion is the amount of heat required to change the phase from solid to liquid or vice versa.

    Latent heat or enthalpy of evaporation is the amount of heat required to convert saturated liquid to

    saturated vapor; it is the amount of heat required to change saturated liquid to saturated vapor at

    constant temperature without changing the pressure.

    Sensible heat is the amount of heat required to change the temperature without changing the pressure.

    Critical point is a point in which liquid and vapor are coexisted in equilibrium.

    Critical pressure is the existing pressure at the critical point. Critical temperature is the temperature at

    the critical point corresponding to an existing critical pressure.

    o For water, critical pressure, pc = 22.09 MPaa, and critical temperature, tc = 374.14oC.

    Triple point is a point in which the melting and boiling or saturation temperature are the samecorresponding to the existing pressure.

    o For water, at triple point: p = 0.6113 kPaa and t = 0.01oC

    Sublimation is the process in which solid will directly change from solid to vapor at a temperature

    corresponding to an existing pressure.

    o For water, sublimation process will occur at p = 0.260 kPaa and t = - 10 oC. Super critical condition is a condition above the critical point (p > 22.09 kPaa for water). This is a

    condition where there is no liquid or vapor phase of pure substance existing in equilibrium.

    The thermodynamic properties considered in the study of pure substance are:

    P = Pressure, MPaa, psia T = Temperature, oC, oF v = Specific volume, m3/kg, ft3/lb u = Specific Internal energy, kJ/kg, Btu/lb

    h = Specific Enthalpy, kJ/kg/ Btu/lb s = Specific Entropy, kJ/kg-oK, Btu/lb-oR

    DIAGRAMS Diagrams hereto are graphical representation of the relation of thermodynamic properties for the

    change of phase at constant pressure such as pV, TV, Ts, pT, and ph diagrams.

    Figure 1.2. Tv Diagram

    o

    SH

    oSC

    Vvgvf

    f x

    sc

    shSuperheated temperature, tsh

    Saturation temperature, tsat

    Subcooled temperature, tsc

    Pressure, p, line

    Saturated LiquidCurve

    cp

    Saturated VaporCurve

    T

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    Thermodynamics 2 Lesson 1

    From Figure 1.2 above,

    Point sc is subcooled liquid condition Point f is saturated liquid condition Point x is wet vapor condition Point g is saturated vapor condition Point sh is superheated vapor condition Point cp is critical point condition oSH = tsh tsat oSC = tsat tsc

    Figure 1.3. pV Diagram

    V

    p

    f

    gx sh

    sc

    Existing pressure or

    Saturation pressure, p, line

    Superheated

    Temperature, tsh

    SaturationTemperature, tsat

    cp

    Subcooled liquid

    Temperature, tsc

    Figure 1.4. Ts Diagram

    ptp

    p

    tsb

    S-L

    L-V

    oSC

    oSH

    Sublimation

    Triple Point

    gf x

    sh

    sc

    t

    tsh

    tsc

    tmp

    ttp

    tc cppc

    Saturated VaporCurve

    Saturated Liquidcurve

    T

    psb

    s

    From Figure 1.4 above

    tmp = melting point temperature ttp = triple point temperature tsb = sublimation temperature ptp = triple point pressure psb = sublimation pressure pc = critical point pressure tc = triple point temperature p = existing or applied pressure

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    Thermodynamics 2 Lesson 1

    Figure 1.5. hs Diagram

    p

    tsat

    g

    f

    sh

    sc

    tsh

    tsct

    cp

    h

    s

    Figure 1.6. pT Diagram

    Triple Point

    Critical Point

    Vapor

    Solid

    Liquid

    EvaporationMelting

    Sublimation

    Sublimation Curve

    Evaporation

    Curve

    Fusion

    Curve

    T

    p

    From figures above

    f stands for saturated liquid g stands for saturated vapor fg stands for evaporation or process from f to g Evaporation (fg) the process of boiling, liquid to vapor phase Condensation (gf) the process of opposite direction, from vapor to liquid Saturated liquid curve is the locus of all states of saturated liquid. Saturated vapor curve is the locus of all states of saturated vapor. Triple point is the state in which three phases may all be present in equilibrium. Enthalpy of sublimation, hig,- is the heat of sublimation or the amount of heat required to

    sublimate the substance.

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    Thermodynamics 2 Lesson 1

    Quality of Vapor/Steam; xo Quality of vapor/steam or dryness factor is the ratio of the mass of vapor content in the mixture to

    that of the mass of the mixture of vapor and liquid.

    %100mm

    mx

    gf

    g

    +=

    Moisture Content; yo Moisture content is amount of saturated liquid in the mixture of saturated vapor and saturated

    liquid; it is the ratio of the mass of saturated liquid to that of the mass of the mixture of saturated

    liquid and saturated vapor.

    %100mm

    my

    gf

    f

    += Note: %100yx =+

    Figure 1.7. Quality of vapor

    mf mg

    Q

    Where, mf= mass of saturated liquid content, kg, lb.

    mg = mass of saturated vapor content, kg, lb.

    x = quality of vapor or steam, or dryness factor, %

    y = moisture content, %

    THERMODYNAMIC PROPERTIES OF EACH STATE

    For Subcooled or Compressed Liquid

    To obtain the properties v, u, h, & s, p and t must be given. Properties are obtained from steam tables if the given substance is water. Values of properties for subcooled liquid must be lower than the properties of saturated

    liquid as indicated in the following relations:

    215 x 10

    -3m

    3/kg

    Therefore, the condition is superheated vapor. Ans.

    h. For p = 1.5 MPaa & oSH = 152.01 oCSince the given temperature is

    oSH, then from steam tables, at 1.5 MPaa,

    t = tsat +o

    SH = 198.32 + 152.01 = 350.33o

    C > tsatTherefore, the given condition is superheated steam. Ans.

    i. For p = 5 MPaa & oSC = 65.43 oCSince the given temperature is

    oSC, then from steam tables, at 5 MPaa,

    t = tsat -oSH = 263.99 65.43 = 198.65

    oC < tsat

    Therefore, the given condition is subcooled liquid. Ans.

    j. For p = 0.35 Mpaa and v = 850 x 10 -3 m3/kgFrom steam tables, at p = 0.35 MPaa,

    vg = 524.3 x 10-3

    m3/kg

    v > vg = 850 x 10-3

    m3/kg > 524.3 x 10

    -3m

    3/kg

    Therefore, the given condition is superheated vapor/steam. Ans.

    Ex. # 1.3] For water as a pure substance and using steam tables, determine the:a. p & u if t = 200 oC and h = 852.45 kJ/kgb. t & h if p = 150 kPaa and u = 1000 kJ/kgc. u & h if p = 800 kPaa and t = 300 oCd. u & h if p = 5 000 kPaa and t = 200 oCe. t & h if p = 300 kPaa and v = 0.850 m3/kg

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    Thermodynamics 2 Lesson 1

    Solution:

    a. For the values of p & u if t = 200 oC & h = 852.45 kJ/kg

    fg

    tsat

    tsh

    p

    T

    s

    Superheated

    Vapor

    x

    sc

    WetVapor

    Saturated

    Vapor

    Saturated

    Liquid

    Subcooled

    Liquid

    From Steam tables, at t = 200oC, hf= 852.45 kJ/kg.

    Since h = hf= 852.45 kJ/kg, water is at saturated liquid condition.

    Therefore, from steam tables, at t = 200oC,

    p = psat = 1.5538 MPaa and u = uf= 850.65 kJ/kg ans.

    b. For the values of t & h if p = 0.15 MPaa and u = 1000 kJ/kgAt p = 0.15 MPaa, uf= 466.94 kJ/kg and ug = 2519.7 kJ/kg

    Since uf< u < ug, water is at wet vapor condition.

    From steam tables, at p = 0.15 MPaa,

    uf= 466.94 kJ/kg ufg = 2052.7 kJ/kghf= 467.11 kJ/kg hfg = 2226.5 kJ/kg

    tsat = 200oC

    For quality x, f

    fg

    u u 1000 466.94x 100% 100% 25.97%

    u 2052.7

    = = =

    Then, ( )f fgh h x h 467.11 0.2597 2226.5 1045.33kJ / kg= + = + = ans

    ans.C37.111tto

    sat ==

    c. For the values of u & h if p = 0.80 MPaa and t = 300 oCAt p = 0.80 MPaa, tsat = 170.43

    oC

    Since tsat < t, the water is superheated steam.

    From steam tables, at p = 0.80 MPaa & t = 300oC,

    u = 2797.2 kJ/kg and h = 3056.5 kJ/kg ans.

    d. For the values of u & h if p = 5 MPaa and t = 200 oCAt p = 5 MPaa, tsat = 263.99

    oC.

    Since tsat > t, the water is subcooled liquid.

    From steam tables (table 4), at p = 5 MPaa and t = 200oC,

    u = 848.1 kJ/kg and h = 853.9 kJ/kg ans.

    e. For the values of u & h if p = 0.30 MPaa and v = 850 x 10 -3 m3/kgAt p = 0.30 MPaa, vg = 605 x 10

    -3m

    3/kg.

    Since v > vg, water is superheated steam.

    From steam tables (table 3), at p = 0.30 MPaa and v = 850 x 10-3

    m3/kg, and

    Using interpolation,

    t,oC V 10

    3m

    3 /kg u, kJ/kg h, kJ/kg

    280 843.8 2775.4 3028.6

    T 850 u h

    290 859.6 2791.1 3048.9

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    Thermodynamics 2 Lesson 1

    Interpolating,t 280 850 843.8 u 2775.4 h 3028.6

    290 280 859.6 843.8 2791.1 2775.4 3048.9 3028.6

    = = =

    t = 283.92oC

    u = 2781.56 kJ/kg and h = 3036.57 kJ/kg ans.

    Ex. # 1.4] An 100-liter tank containing a mixture of saturated liquid water and saturated steam at 370

    o

    C. a)Find the mass of each phase if their volumes are equal. b) Find the volume occupied by each phase if theirmasses are equal.

    Given: 100-liter tank with saturated water and steam

    t = 370oC

    Required:

    a. mf& mg if Vf= Vg

    Vg

    Liquidt = 370

    oC

    Va or

    b. Vf& Vg if mf= mg

    Solution:

    a. For the values of mf& mg if Vf= VgmgFrom steam tables at t = 370 oC,

    vf= 2.213 x 10-3

    m3/kg Vf mfvg = 4.925 x 10

    -3m

    3/kg

    Considering the total volume,3T

    gf m05.02

    VVV ===

    Therefore, kg59.22kg/m10x213.2

    m05.0

    v

    Vm

    33

    3

    f

    ff === ans

    kg15.10kg/m10x925.4

    m05.0

    v

    Vm

    33

    3

    g

    g

    g === ans.

    b. For the values of Vf& Vg if mf= mgFrom steam tables at t = 370 oC,

    vf = 2.213 x 10-3

    m3/kg

    vg = 4.925 x 10-3

    m3/kg

    Considering the mass,gf

    f g

    f g

    VVm m

    v v= =

    Then, ggg

    fgf V44934.0V

    925.4

    213.2

    v

    vVV =

    =

    = eq. 1

    Liquid

    Vapor

    t = 370oC

    Vg mg

    Vf mf

    Considering the volume, 10.0VVV Tgf ==+

    gf V10.0V = eq. 2

    Equating eq. 1 and eq. 2, gg V10.0V44934.0 =

    3g m069.0

    44934.1

    10.0V == ans

    Then, ans3

    gf m031.0069.010.0V10.0V ===

    Ex. # 1.5] Determine the volume occupied by 2.25 kg steam at 8 MPaa and 60 % quality.

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    Thermodynamics 2 Lesson 1

    Given: Wet steam

    m = 2.25 kgp = 8 MPaa

    Saturated

    LiquidSaturated

    Va or

    x = 60 %

    Required:

    The volume occupied by the wet vapor.

    Solution:

    From steam tables, at p = 8 MPaa,

    vf= 1.3842 x 10-3

    m3/kg and vg = 23.52 x 10

    -3m

    3/kg

    For the specific volume of wet vapor,

    ( ) ( )[ ] 3fgf 103842.152.2360.03842.1vvxvv +=+=

    v = 14.66568 x 10-3

    m3/kg

    Then, for the volume occupied by the 2.25 kg wet vapor,

    ( ) liters33m033.010x66568.1425.2vmV 33 ====

    Ex. # 1.6] A rigid container with a volume of 2 000 liters contains 4-kg mixture of saturated water andsteam at 120

    oC. The mixture is slowly heated until the liquid content is completely vaporized. Determine

    the a) quality of the vapor at the initial condition; and b) temperature of water after heating.

    Given: A rigid tankVT = 2 000 liters = 2 m

    3m = 4 kg t1 = 120

    oC

    x2 = 100 %

    Required:

    a. The initial quality of vaporb. The final temperature

    V1 = V2

    2

    1

    t2

    t1 =120oC

    Figure:T

    Rigid

    ContainerVapor

    Liquid

    QVSolution:

    From steam tables, at t1 = 120oC,

    vf1 = 1.0603 x 10-3

    m3/kg

    vg1 = 891.9 x 10-3

    m3/kg

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    Thermodynamics 2 Lesson 1

    Solving for the initial specific volume of the mixture,

    kg/m10x500kg/m5.0kg4

    m2

    m

    Vv 333

    31

    1====

    a. For the quality of steam at initial condition

    ( ) ( ) %01.56%1000603.19.891

    0603.1500%100

    v

    vvx

    1fg

    1f11 =

    =

    =

    b. For the final temperature after heatingSince the container is rigid, the volume does not change during the process.

    v2 = v1 = vg2 = 500 x 10-3

    m3/kg

    From steam table (table 1), at v2 = 500 x 10-3

    m3/kg and x2 = 100 %

    T, C vg, m3/kg

    140 508.9 x 10-3

    t 500 x 10-3

    141 495.6 x 10-3

    Interpolating,t 140 500 508.9

    141 140 495.6 508.9

    =

    Then, ( ) o500 508.9

    t 141 140 140 140.67 C495.6 508.9

    = + =

    Ex. # 1.7] A piston-cylinder arrangement contains 100 liters of saturated water and 900 liters of saturated

    steam in equilibrium at 1 MPaa. Heat is added at constant pressure until the temperature becomes 300oC.

    Determine a) the initial temperature; b) the total mass; c) the quality of vapor at initial condition; d) thefinal volume; and e) the work done during the process.

    Given: A piston-cylinder device

    Vf1

    Vg1

    Q

    Vf1 = 100 liters = 0.10 m3

    Vg1 = 900 liters = 0.90 m3

    p1 = p2 = 1 MPaat2 = 300

    oC

    Required:

    a. Initial temperatureb. Total massc. Quality of steam at initial conditiond. Final Volumee. Work done during the process

    Solution:

    a. For the initial temperature

    From steam tables, at 1 MPaa,

    t1 = tsat = 179.91oC

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    Thermodynamics 2 Lesson 1

    b. For the total mass

    At 1 MPaa, vf1 = 1.1273 x 10-3

    m3/kg and vg1 = 194.44 x 10

    -3m

    3/kg

    Then,3

    f1f1 3 3

    f1

    V 0.10 mm 88.71 kg

    v 1.1273 x10 m / kg

    = = =

    3g1

    g1 3 3

    g1

    V 0.90 mm 4

    v 194.44 x10 m / kg= = = .63 kg

    Therefore, the total mass will be

    kg34.9363.471.88mmmm 21g1f1 =+==+=

    c. For the quality of vapor

    g1

    1

    1

    m 4.63x 100 % 100% 4.96 %

    m 93.34

    = = =

    d. For the final volume

    At point 2, p2 = 1 MPaa and t2 = 300oC

    v2 = 257.9 x 10-3

    m3/kg

    Then, ( )3 3 32 2 2V m v 93.34kg 257.9x10 m / kg 24.07 m= = =

    e. For the work done during the process

    ( )122

    1

    2

    1VVpdVpdVpW ===

    ( )W 1000 24.07 1.0 23070 kJ= =

    IMPORTANT POINTS TO REMEMBER

    Saturation temperature is a temperature at which vaporization of liquid or condensation of vapor

    takes place at a given or existing pressure. Saturation pressure is an existing pressure during the vaporization or condensation of the substance

    at a temperature known as saturation temperature. Sub-cooled liquid is the liquid that has a temperature lower than the saturation temperature

    corresponding to the given or existing pressure. Compressed Liquid, synonymous with sub-cooled liquid, is the liquid that has a pressure higher than

    the saturation pressure corresponding to the existing temperature.

    Saturated liquid is the liquid that has a temperature equal to the boiling point corresponding to theexisting or given pressure.

    Vapor is a substance existing in the gaseous phase but relatively near its saturation temperature. Saturated Vapor is the vapor that has temperature equal to the saturation temperature corresponding

    to an existing pressure. Degree of superheat,

    oSH, is the difference between the temperature of superheated vapor and the

    saturation temperature for an existing pressure. Degrees Sub-cooled,

    oSC, is the difference between the saturation temperature for the given pressure

    and the actual sub-cooled liquid temperature.

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    Thermodynamics 2 Lesson 1

    Wet Vapor is the mixture of saturated vapor and the saturated liquid. Quality of wet vapor, x, is the percentage by weight of vapor in the mixture of saturated vapor and

    saturated liquid. Percent Moisture, y, is the percentage by weight of liquid in the mixture of saturated liquid and

    saturated vapor. Latent Heat of Evaporation is the amount of energy required to convert saturated liquid to saturated

    vapor or from saturated vapor to saturated liquid with the temperature remains constant.

    Sensible heat is the amount of heat required to change the temperature of a substance without

    changing the phase. Critical point is a point that represents the highest pressure and highest temperature at which liquid

    and vapor can coexist in equilibrium.

    PROBLEMS

    Prob. # 1] Determine the properties and draw the Tv, pV, Ts, & hs diagrams of water for the following

    conditions:

    a) t = 102 oC & saturated liquidb) p = 700 kPaa & x = 100 %c) t = 70 C & x = 80 %d) p = 0.5 MPaa & h = 2895.6 kJ/kge) p = 0.356 MPaa & t = 321.67 oC

    Prob. # 2] Specify the condition (subcooled liquid, saturated liquid, wet vapor, etc.) of water for the

    following conditions. Justify your answer and show pV and Ts diagrams for each item.a. p = 900 kPaa & v = 1.0245 x 10-3 m3/kgb. t = 76 C & u = 3542.2 kJ/kgc. t = 100 oC and p = 2.5 Mpaad. p = 1.2 MPaa & oSH = 234.6 oCe. p = 1 Mpaa & oSC = 100 oC

    Prob. # 3] A pumping discharging water at 1 MPaa and 165oC. Determine the specific volume and internal

    energy of the water at the pump discharge.

    Prob. # 4] A 500-liter tank contains saturated mixture of water at 300 kPaa. If the saturated liquid occupies10 % of the volume, determine a) the the quality of vapor, and b) the total mass of water in the tank.

    Prob. # 5] A piston-cylinder device initially contains 300 liters of water at 420 kPaa and 110oC. Heat is

    added to the water at constant pressure until the liquid is entirely vaporized. Determine a) the mass of

    water; b) the final temperature; c) the final volume of water; d) the work done during the process; and e)

    the amount of heat added.