1 On which side of the Coors Event Center arena will the PHYS2010 final exam take place? A)North...

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1 On which side of the Coors Event Center arena will the PHYS2010 final exam take place? A) North B) South C) East D) West E) I don’t know! Clicker Question Room Frequency B Flatirons are west of campus!

Transcript of 1 On which side of the Coors Event Center arena will the PHYS2010 final exam take place? A)North...

Page 1: 1 On which side of the Coors Event Center arena will the PHYS2010 final exam take place? A)North B)South C)East D) West E) I don’t know! Clicker Question.

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On which side of the Coors Event Center arena will the PHYS2010 final exam take place?

A) NorthB) SouthC) EastD) WestE) I don’t know!

Clicker Question Room Frequency BA

Flatirons are west of campus!

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• CAPA assignment #15 is due on tonight at 10 pm.

• By Sunday final Clicker scores will be posted on CULearn

• By Monday all Recitation/Lab scores will be posted.

• If you find a discrepancy, send me email Monday evening to [email protected]

Announcements

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• Final Exam is Tuesday morning, Dec 13, 10:30am – 1pm

• Exam will be held in Coors Event Center, on the West (mountain) side of the arena. Calc-based physics is on the east side; don’t sit down in the wrong side!

• We are in sections 20, 21, 22, with individual seat assignments. Your seat assignment are posted on CU Learn.

• Bring student ID. We will be checking that people are in their assigned seat.

• Practice Exams and Formula sheet are posted on CULearn; you can ignore Prob. 37 on the practice exam

Final Exam News

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Solving Calorimetry Problems

• Problem solution is based on energy conservation: heat lost by hot object must equal heat gained by cold object• Heat (transfer without phase change) Q = mcΔT• Latent Heat (Phase change) Q = mL• In problems with phase changes, you have to figure out the final phase or phases• Final state can be all one phase or a mixture of several phases

QMatter cooling off =QMatter heating up

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An ice cube is placed in a cup containing some liquid water. The water and ice exchange energy with each other but not with the outside world. After the water and ice come to the same temperature, is it possible the ice could freeze the water rather than the water melt some of the ice?

A) Yes, the ice could freeze the water.B) No, the water will always melt some of the ice.

Clicker Question Room Frequency BA

If the ice is cold enough initially (well below zero), then the heat lost by the liquid to cool it and freeze it could be more than the heat gained by the initial cold ice!

liquid water

ice

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Calorimetry Example with Ice - 11 kg of ice at temperature -200°C is placed is a container of 100 mL of water at 20°C. What is the final temperature and phase of the system?

Preliminary analysis: Will the final state be all ice, all water or a mixture of ice and water?

Energy gain to heat ice to 0°C: Qice=micecice(200-0) with cice = 2100 J/(kg°C) and mice = 1 kg, Qice = 420,000 J Ice will heat up, water will cool to 0°C and start to freeze;

how much of the water will freeze? Look at total water freeze.

Qwater to ice = mwaterLice-water = 0.1 kg*333,000 = 33,000 J

Energy loss to cool water to 0°C: Qwater=mwatercwater(0-20) with cwater = 4186 J/(kg°C) and mwater = 0.1 kg, Qwater = 8372 J

Original ice would gain 8372+33,000 J = 41372 J < 420,000 J Not enough to bring ice up to 0°C => All ice in the final state

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Calorimetry Example with Ice - 21 kg of ice at temperature -200°C is placed is a container of 100 mL of water at 20°C.

Qice=micecice(Tf - -200) cice = 2100 J/(kg°C)

Using cwater = 4186 J/(kg°C), Lwater-ice = 333,000 J/kg

|Qice| =micecice(Tf + 200 ) = |Qwater| =mwatercwater(20) + mwaterLwater-ice

+ mwatercice(0 – Tf ) Solve for Tf and You’ll get

Qwater=mwatercwater(0-20) - mwaterLwater-ice + mwatercice(Tf - 0)

T f =mwatercwater20 +mwaterLwater−ice−micecice200

cice(mice+mwater )

Tf = -164°C Is the final T between -200 and 0? Yes!

Final analysis: Final state will be all ice. What is Tf?

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Calorimetry Example with Less Ice - 10.05 kg of ice at temperature -200°C is placed is a container of 100 mL of water at 20°C. What is the final temperature/phase of the system?

Preliminary analysis: Will the final state be all ice, all water or a mixture of ice and water?

Energy gain to heat ice to 0°C: Qice=micecice(0 - -200) with cice = 2100 J/(kg°C) and mice = 0.05 kg, Qice = 21,000 J Ice will heat up, water will cool to 0°C and start to freeze;

how much of the water will freeze? Look at total water freeze.

Qwater to ice = mwaterLice-water = 0.1 kg*333,000 = 33,000 J

Energy loss to cool water to 0°C: Qwater=mwatercwater(0-20) with cwater = 4186 J/(kg°C) and mwater = 0.1 kg, Qwater = 8372 J

Heat Loss to freeze all water is 8372+33,000 J = 41372 J > 21,000 J Not enough to freeze all water => Ice water mixture in the final state

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Calorimetry Example with Less Ice - 2

Qice=micecice(0 - -200) cice = 2100 J/(kg°C)

Using cwater = 4186 J/(kg°C), Lwater-ice = 333,000 J/kg

|Qice| =micecice(200 ) = |Qwater| =mwatercwater(20) + mfreezeLwater-ice

Solve for mfreeze :

Qwater=mwatercwater(0-20) - mfreezeLwater-ice + mwatercice(0 - 0)

m freeze =micecice200−mwatercwater20

Lwater−ice

mfreeze = 0.038 kg Must be less than original 0.1 kg of water

Final analysis: Final state will be ice-water mixture (at 0 °C). How much ice and water will there be?

mtotal-ice = 0.088 kg, mliquid water = 0.062 kg (62 mL)

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Gases and Absolute Temperature• In 1600’s Robert Boyle find gas Pressure P times its Volume V is a constant at constant temperature: PV = constant• In late 1700’s Jacques Charles find that at constant pressure, the Volume of the gas changes linearly with temperature T(°C) giving V = constant*(T+267)• Inventing a new temperature scale Tabs = T(°C) +267, we get Charles’ law V = constant * Tabs

• In early 1800’s, Joseph Gay-Lussac finds Pressure P is proportional to T(K): P = constant*Tabs

• In 1834 Clapeyron put all this together to get PV = nRTabs

• R is the same for many gases! n is “amount” of gas• Avogadro says n is the number of molecules• 1 mole = 6.02 x 1023 molecules• More refined Tabs is Kelvin scale T(K) = T(°C) + 273.15

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Gas Constants• In SI units, R = 8.314 J/(mole*K)• If you want to see this law in terms of individual gas molecules, you divide R by Avogadro’s number to get k, the Boltzmann constant• In SI units, k = 1.38 x 10-23 J/K• Now Ideal Gas Law is PV = NkT, where N is the number of gas molecules• In many problems, N is a constant, so we have PV/T = constant

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A balloon full of gas of volume 1 m3 at pressure 1 atm at temperature 20°C. If I heat the balloon to 40°C and double the pressure to 2 atm, what is the approximate volume of the balloon?

A) 0.5 m3

B) 1.0 m3

C) 2.0 m3

D) 4.0 m3

E) None of the above

Clicker Question Room Frequency BA

PV/T = constant = (1 atm)(1 m3)/293 K = (2 atm)(V)/313 K

V =(313/293)/2 m3 = 0.534 m3

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Mechanics and Ideal Gas Law• Consider a hollow cube of side length L filled with N atoms• Each atom has mass m and average velocity v• If the atoms bounces off a wall of the cube it exerts a force on the wall, and the wall exerts a force on the atom

Lv

F

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Atom Force on Wall• The average force is found from the change in the atom momentum FaveΔt = mΔv ≈2mv, so Fave = 2mv /Δt (single atom)• For N atoms in cube, about 1/6 are heading towards a given wall• Then on average for Δt = L/v ,N/6 hit the wall each giving an average force Fave .• Average total force FT on a wall is then (N/6)*(2mv)/(L/v) = Nmv2/3L • Pressure P = FT/L2 = Nmv2/3L3 • P = Nmv2/3V or

• PV = N(2/3)(mv2/2) = N(2/3)(KEatom)

v

FΔv ≈ 2v

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Kinetic Theory!• PV = NkT from experiment• PV = N*number*KE from theory of molecules

• kT is average kinetic energy of molecules!!!

• Using proper exact averages you find 12 mv

2 = 32 kT

• In a real gas, there is a distribution of velocities• square root of average of v2 is called vrms and we now get formula

vrms = v2 =3kTm

.

At same T, molecule speed is faster for lighter molecules

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Two boxes, one filled with helium (m = 4u) and one filled with nitrogen (m =30 u) are brought to the same temperature T. The box holding nitrogen is twice as large as that holding helium.

How are the average kinetic energies of the individual molecules of the two gases related? A) KEHe < KEN

B) KEHe = KEN

C) KEHe > KEN

D) not enough information

Clicker Question Room Frequency BA

3kT/2 = average KE so same T, same average KE

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Two boxes, one filled with helium (m = 4u) and one filled with nitrogen (m =30 u) are brought to the same temperature T. The box holding nitrogen is twice as large as that holding helium.

How are the average molecular speeds of the two gases related? A) vHe < vN

B) vHe = vN

C) vHe > vN

D) not enough information

Clicker Question Room Frequency BA

Nitrogen is heavier, hence vN is smaller

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On behalf of Profs. Nagle and Uzdensky

Thank you for being a great class!

Stay calm and rested and do well on the final exam!!!