thermodynamics prepared by: engr. darwin mañaga

49
1 1 Maxim Confidential THERMODYNAMICS Prepared by: Engr. Darwin Mañaga

Upload: pippa

Post on 11-Jan-2016

157 views

Category:

Documents


0 download

DESCRIPTION

THERMODYNAMICS Prepared by: Engr. Darwin Mañaga. Thermodynamics – transformation of heat energy into other forms of energy and vice versa. Forms of Energy Heat ; Q Potential ; PE Kinetic ; KE Internal ; U Flow ; W f Enthalpy ; H = U + W f Mechanical Work ; W. - PowerPoint PPT Presentation

TRANSCRIPT

Page 1: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

11Maxim Confidential

THERMODYNAMICS

Prepared by: Engr. Darwin Mañaga

Page 2: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 2

Thermodynamics – transformation of heat energy into other forms of energy and vice versa

Page 3: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 3

Forms of Energy

1. Heat ; Q

2. Potential ; PE

3. Kinetic ; KE

4. Internal ; U

5. Flow ; Wf

6. Enthalpy ; H = U + Wf

7. Mechanical Work ; W

Page 4: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 4

Power ; P = energy / unit time

Energy ; E = the ability or capacity to do work

Work = Force*distance ( always parallel to the axis of motion )

Page 5: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 5

Unit of Power

English MkS-cgs SI

1 hp = 1 eng hp = 1 arabian horse

1 french horse = 1 Chueval Vapuer

Watt, J/s, Nm/s

1 mule = 1 mola 1 Pfer Starkey

1 hp = 550 lbf – 1 ft / sec

= 33000 lbf – 1 ft / min

1 met hp = 75kgs – m/1 sec

Page 6: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 6

Energy Units Conversions

English MKS SI

BTU Cal J

Ft-lbf Dyne-cm N-m

Therm erg

Page 7: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 7

Conversion of Energy Units

1 BTU = 778.16 ft-lbf 1 kgf = 9.8066 N1 BTU = 1.055 KJ 1 erg = 1 dyne -

cm1 J = 1 N-m1 J = 107 dyne-cm1 J = 107 erg1 cal = 4.18 J

1 lbf = 4.4482 N

Page 8: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 8

Heat Energy ; Q

Qs = sensible heat = MCp(t2-t1)

Cp - specific heat at constant pressure

QL = latent heat ( only phase change )

- solid to liquid:

QL = mhfi ; hfi – latent heat of fusion of ice

hfi = 144 BTU/lbm = 8000Kcal/kgm = 335 KJ / kgm

- liquid to gas:

QL = mhfg ; hfg – latent heat of fusion of air

hfg = 970.3 BTU/lbm = 540Kcal/kgm = 2257 KJ / kgm

Page 9: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 9

Kinetic Energy – due to velocity

KE = 0.5 mv2/k ; k – proportional constant

eng mks SI

1 slug-ft/lbf-s2 = 1 gm – cm/dyne - s2 = 1 kgm – m/N - s2 =

32.174 lbm – ft/lbf-s2 = 9.8066 kgm – m/kgf - s2 = 9.8066 kgm – m/kgf - s2

Page 10: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

1010Maxim Confidential

1. If the mass of a typical neutron is 1.66x10-24 gram and the velocity is approximately 2200m/s. What is the kinetic energy of this neutron in electron volt. Note: 1 ev = 1.6x10-

12 erg.

a. 1.025b. 0.025c. 0.889d. 1.228

Page 11: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 11

2. The ratio of the density of a substance to the density of some standard substance is called

a. relative densityb. specific gravityc. specific densityd. relative density

Page 12: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 12

3. The S.I unit of force

a. poundb. Newtonc. kilogramd. Dyne

Page 13: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 13

Remember the conversions:

1 pound = 1 lb

1 pond = 1 gram

1 poundal = 32.174-1 pound

Page 14: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 14

4. Heat normally flowing from a high temperature body to a low temperature body wherein it is impossible to convert heat without other effects is called

a. second law of thermodynamicsb. first law of thermodynamicsc. third low of thermodynamicsd. zeroth law of thermodynamics

Page 15: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 15

Laws of Thermodynamics:

1st Law: Law of conservation of energy

- Energy can neither be created nor destroyed but it can be transformed from on form to another

Ein = Eout

Page 16: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 16

2nd Law: Law of degradation of energy

- Heat is moving from heat body to cold body

- No engine w/ 100% thermal efficiencyn = (W/QA)x100% = ((QA – QR)/QA)*100%

= ((TMAX – TMIN)/ TMAX)*100%

Note:

Use absolute temp for T

R = deg F + 460 ; K = deg C + 273

Page 17: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 17

3rd Law: Law of absolute zero temperature

- @ absolute zero temp. line, all molecules of a crystalline substance are dead & the degree of disorder of molecules is equal to 0 & heat is eventually equal to 0.

Page 18: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 18

Zeroth or 4th Law:

- made by Filipino

- keyword: 3rd body

Page 19: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 19

Potential Energy – due to elevation

= Weight*distance ; N*m or J

Page 20: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 20

5. The weight of a 100kg mass body at a given elevation is 0.9804kN. If the variation from the standard gravitational acceleration is –0.004mps2 per 1000m. Determine the elevation at this point.

a. 550mb. 50mc. 660md. 650m

Page 21: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 21

Pressure

Pabs = Pbaro + Pg = Pbaro – Pvac

Note:

If Pbaro is not mentioned, use Pbaro = 1 atm

Page 22: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 22

Pressure Conversions:Eng Mks SI

14.7 lbf/in2 = 1.0332 kgf/cm2 = 101.325 kPa or KN/m2 =

29.92 inHg = 760 mmHg = 0.76 mHg =

34 ftH20 = 10330 mmH20 = 10.33 mH20

Page 23: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 23

Remember:

1 TORR = 1mmHg

1 bar = 100kPa

Page 24: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 24

6. The pressure of a boiler is 9.5 kg/cm2 . The barometric pressure of the atmosphere is 768mm of mercury. Find the absolute pressure in the boiler in MPa.

a. 1.03b. 2.03c. 3.03d. 4.03

Page 25: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 25

7. How many metric horse power are there in 10 kW?

a. 13.4b. 13.59c. 15.16d. 16.33

Page 26: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 26

8. A pressure of 1 millibar is equivalent to

a. 1000 dynes/cm2

b. 1000 cm Hgc. 1000psid. 1000kg/sq.cm

Page 27: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 27

8. What is the minimum pressure required to force blood from the heart to top of the head if the vertical distance is 27 in? Assume the density of the blood to be 1.04gm/cm3 and neglect friction. Express the answer in mmHg.

a. 54.42b. 52.44c. 42.25d. 25.54

Page 28: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 28

Remember:

Pressure in mmHg = (Specific Gravity of substance)(h)

13.6

Page 29: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 29

9. A water temperature rise of 18 deg F in the water cooled condenser is equivalent in deg C to

a. -7.78b. 10c. 265.56d. -9.44

Page 30: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 30

10. If the temperature is held constant and increased beyond the saturation pressure, we have a

a. saturated vaporb. compressed liquidc. saturated liquidd. sub-cooled liquid

Page 31: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 31

Flow Energy ; Wf

- aka resistance energy

Wf = (Pressure)(Volume)

Page 32: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 32

11. A piston was moved at a distance of 75cm by a gas pressure of a 450kPa. If the work done is 15kJ, the piston diameter in cm is

a. 23.79b. 27.93c. 29.37d. 32.79

Page 33: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 33

12. The change of water from the solid to vapor phase.

a. always must occur in two steps-solid to b. liquid to liquid then liquid to vaporb. can occur directly at elevated pressurec. can occur directly at extremely low pressured. can occur directly at room temperature

Page 34: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 34

13. Which of the following is an example of path function?

a. temperatureb. volumec. workd. entropy

Page 35: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 35

Point Functions

• Temp

• Pressure

• Volume

• Entropy

• Internal energy

• Enthalpy

Path Functions

• Heat

• Work

Page 36: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 36

14. What is the process if n = negative to positive infinity?

a. isobaricb. isothermalc. polytropicd. isentropic

Page 37: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 37

General Equation:

PVn = C

0 1 K -∞ to + ∞ + ∞

Isobaric/Isopiestic

Isothermal Isentropik/reversible adiabatic

Polytropic Isometric/Isochoric/

Isovolumeric

Page 38: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 38

15. In a sealed and rigid system, the constant is

a. volumeb. pressurec. temperatured. entropy

Page 39: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 39

17. In a sealed and rigid system, determine the output atmospheric pressure if the input atmospheric pressure is 2 atm. The temperature at the input is 27 deg C w/c increases to 100 deg C at the output.

a. 0.725 atmb. 0.625 atmc. 0.825 atmd. 0.925 atm

Page 40: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 40

18. Non flow work is applicable to

a. closed systemb. open systemc. impact systemd. solar system

Page 41: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 41

Work

Non Flow Work:

Wn = ∫ Pdv

Steady Flow Work:

Ws = - ∫ Vdp

Page 42: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 42

NFW (Closed System)

• Piston

- mass will not cross the boundary

SFW (Open System)

• Turbine

• Pump

- mass and energy cross the boundary

Page 43: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 43

19. Pressure of octane and air were mixed and produced 86.1 kPa. Determine the pressure of air considering the following parameters: mass of octane = 0.0624 kg. R of octane = 8.314/114; mass of air = 0.91 kg. R of octane = 8.314/29. At a temperature of 290 K.

a. 84.6 kPab. 94.6 kPac. 64.6 kPad. 44.6 kPa

Page 44: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 44

Daltons Law

- mixture of gases is equal to the summation of the pressures

PTOTAL = ∑ P = P1 + P2 + P3 . . . + PN

Page 45: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 45

20. A 20x10-3 kg bullet running at 250m/sec hit a target and travelled 12 cm after the impact. Determine the force.

a. 4280Nb. 5280Nc. 6280Nd. 7280N

Page 46: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 46

Internal Energy; U- due to the movement of molecules

U = mCV(t2 – t1)

Page 47: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 47

Enthalpy; U- sum of internal energy and flow energy

H = U + Wf = mCpt + PV = mCp(t2 – t1)

Page 48: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 48

Mechanical work or energy ; W- due to shaft rotation or piston movement

W = (force)(distance)

ω = (Frequency of rotation)(radius) = Torque = rad/sec

Power = (Torque)(ω) = watt

Page 49: THERMODYNAMICS  Prepared by: Engr. Darwin Mañaga

Maxim Confidential 49