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Announcements 9/20/10

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Announcements 9/20/10. Demo: constant volume change (hopefully working today) Do this “Quick Writing” assignment while you’re waiting: - PowerPoint PPT Presentation
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Announcements 9/20/10 Demo: constant volume change (hopefully working today) Do this “Quick Writing” assignment while you’re waiting: Ralph is confused because he knows that when you compress gases, they tend to heat up (think of bicycle pumps). So, how are “isothermal” processes possible? How can you compress a gas without its temperature increasing?
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Page 1: Announcements 9/20/10

Announcements 9/20/10

Demo: constant volume change (hopefully working today)

Do this “Quick Writing” assignment while you’re waiting:

Ralph is confused because he knows that when you compress gases, they tend to heat up (think of bicycle pumps). So, how are “isothermal” processes possible? How can you compress a gas without its temperature increasing?

Page 2: Announcements 9/20/10

Thought question (ungraded)

How will the temperature of the gas change during this process from A to B?

a. Increaseb. Decreasec. First increase, then

decreased. First decrease, then

increasee. Stay the same

0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6 1.8 2.00.0

0.2

0.4

0.6

0.8

1.0

1.2

1.4

1.6

1.8

2.0

Pre

ssur

e (a

tm)

Volume (m3)

A

B

Page 3: Announcements 9/20/10

Reading quiz (graded)

What is “CV”?

a. heat capacity b. mass-pacityc. molar heat capacityd. molar heat capacity, but only for

constant volume changese. a detailed resumé

Page 4: Announcements 9/20/10

Thought question (ungraded)

Which should be larger, the molar heat capacity for constant volume changes or the molar heat capacity for constant pressure changes? (Hint: Think of the First Law.)

a. constant volumeb. constant pressurec. they are the samed. it depends on the temperature

Page 5: Announcements 9/20/10

CV and CP

Constant volume change (monatomic):W = 0Eint = Qadded

(3/2)nRT = Qadded

Compare to definition of C: Qadded = nCVT

(like Qadded = mcT)

CV = (3/2)R Constant pressure change

a. What’s different?b. result: (monatomic) CP = (5/2)R

What would be different for gases with more degrees of freedom?

Page 6: Announcements 9/20/10

Reading quiz (graded)

What does gamma equal in the equation for an adiabatic process:

a. CP + CV

b. CP - CV

c. CV - CP

d. CV / CP

e. CP / CV

constantPV

Page 7: Announcements 9/20/10

Isothermal vs Adiabatic

Isothermal: Adiabatic:

steeper curves for adiabatic

constantPV constantPV

Page 8: Announcements 9/20/10

Thought question

How much do you think the temperature of the air in this room would change by if I compressed it adiabatically by a factor of 10? (Vf = V0/10)

a. less than 0.1 degree Cb. about 0.1 degrees Cc. about 1 degree Cd. about 10 degrees Ce. more than 10 degrees C

Page 9: Announcements 9/20/10

Demo/Video

Video: adiabatic cotton burner Demo: freeze spray Video: adiabatic expansion

Page 10: Announcements 9/20/10

Derivation of PV (for Monatomic)Eint = Qadded + Won

(3/2) nRT = -integral(PdV)(3/2) nRdT = -PdV(3/2) nR d(PV/nR) = -PdV(3/2) (PdV + VdP) = -PdV(3/2) VdP = -(5/2) PdVdP/P = -(5/3) dV/VlnP = (-5/3)lnV + constantlnP = ln(V-5/3) + constantP = constant V-5/3 (it’s a different constant)

P V5/3 = constant

What’s differentif diatomic?

Page 11: Announcements 9/20/10

Thought question Which of the curves on the PV diagram below

is most likely to represent an isothermal compression, followed by an adiabatic expansion back to the initial volume?

a.

b.

c.

d.

e.

Page 12: Announcements 9/20/10

Thought questions What would be the molar specific heat for an

adiabatic process? (Hint: think of Q = nCT.)a. CV

b. CV + Rc. CV + 2Rd. CV - Re. none of the above

What would be the molar specific heat for an isothermal process? (Same hint.)

a. CV

b. CV + Rc. CV + 2Rd. CV - Re. none of the above

Page 13: Announcements 9/20/10

Water/steam “saturation curve”: ideal gas?

0.00 0.01 0.02 0.03 0.04 0.05 0.060

5000

10000

15000

20000

25000

30000

Part Liquid, Part GasAll Liquid

Pre

ssu

re (

kPa

)

Volume, divided by mass (m3/kg)

bk = actual data for water/steam

All Gas

adding heatenergy, T=325C

1 atm= 101 kPa

Page 14: Announcements 9/20/10

Water/steam “saturation curve”: ideal gas?

0.00 0.01 0.02 0.03 0.04 0.05 0.060

5000

10000

15000

20000

25000

30000

Part Liquid, Part GasAll Liquid

Pre

ssu

re (

kPa

)

Volume, divided by mass (m3/kg)

bk = actual data for water/steamrd = ideal gas, T=400bl = ideal gas, T=500gn = ideal gas, T=600

All Gas

adding heatenergy, T=325C

1 atm= 101 kPa

Page 15: Announcements 9/20/10

Water/steam “saturation curve”: ideal gas?

0.00 0.01 0.02 0.03 0.04 0.05 0.060

5000

10000

15000

20000

25000

30000

Part Liquid, Part GasAll Liquid

Pre

ssu

re (

kPa

)

Volume, divided by mass (m3/kg)

bk = actual data for water/steamrd = ideal gas, T=400bl = ideal gas, T=500gn = ideal gas, T=600

All Gas

"critical point"

adding heatenergy, T=325C

1 atm= 101 kPa

Page 16: Announcements 9/20/10

Water/steam “saturation curve”: ideal gas?

0.00 0.01 0.02 0.03 0.04 0.05 0.060

5000

10000

15000

20000

25000

30000

Part Liquid, Part Gas

????

All Liquid

Pre

ssu

re (

kPa

)

Volume, divided by mass (m3/kg)

bk = actual data for water/steamrd = ideal gas, T=400bl = ideal gas, T=500gn = ideal gas, T=600

All Gas

"critical point"

adding heatenergy, T=325C

1 atm= 101 kPa


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