The final exam will take place Wednesday, April 30 at 8 am. The exam will consist of 1 to 12 problems and cover from Chapter 1 through Chapter 20. About half will be over the material from Ch 1-16 and about half over the new material, Ch 17-20. Below are a few sample exam problems for Ch 17-20.
You are responsible for all material covered in lecture and homework assignments. DO NOT ASSUME that a subject not covered in the sample exam below will not show up on Tuesday's exam! During the exam, you will be provided with an equation sheet. You may download the Equation sheet. You will be allowed to use only the equations on the sheet, or others that you derive from those on the sheet. Use only that when trying the problems below. Resist the temptation to look at the answers, as that will better prepare you for the exam.
DVHg = bHgVDT = inner volume of the tube = (pr2)L , -> r = 0.00761 cm without the glass correction
For the bonus, the Hg must fill the glass tube and the increase in volume of the glass bulb:
DVHg = bHgVDT = (pr2)L + 3aglassVDT, -> r = .00741 cm.
Calculate c for the drink from, DQ1 + DQ2 + ... = 0. (100g)c(0-20) + (30gm)(80 cal/gm) = 0, so c = 1.2 cal/gmoC. What effect would assuming that there is some heat loss have on this result? That is, does that assumption imply that this is definitely not Saurian brandy or could it be that it is Saurian Brandy and the heat loss could account for the low result? What other assumption(s) did you have to make?
Since equilibrium is reach after only part of the water boils away, then the final temperature of the metal and remaining 190 gm of water must be 100oC. So our heat conservation equation is"
(100 gm)(c metal)(100-1000) + (200 gm)(1.0 cal/gmoC)(100-20) + (10 gm)(540 cal/gm) = 0. Solve for c metal = 0.24 cal/gmoC
DQDt = kADTDx = (0.008)[2x(1.0x1.0) + 4x(1.0x0.5)][25-(-20)] / 0.05 = 29 Watts
PV = nRT -> (100,000Pa)(.001m3) = n(8.314)(~300K) -> n ~ .04 moles which is .04 x 6.02 x 1023 = 2.4 x 1022 molecules.
1. For the isotherm, DU = 0, DQ = W = nRTln(Vf/Vi). We find T = PV/nR = 3x105(0.025)/1(8.314) = 902, (or just insert PV for nRT), so W = 8200 J which is also DQ.
2. For the isobar, W = P(DV) = 105(0.025-0.075) = -5000 J, DQ = nCpDT. The temperature starts at 902 and drops to 902/3 = 301 and Cp = CV + R = (7/2)R for a diatomic gas, so DQ = - 17,500 J. And finally, we can get DU from nCvDT or DU = DQ - W = -12,500 J.
3. For the isochor, W = 0, and DQ = DU = nCvDT = 1(5/2)R(902-301) = +12,500 J.
Finally, for the whole cycle, simply add each segment. DU = 0 (always!), and the net heat exchange is the work out, DQ = W = 3200 J. Note the net work is positive, as to be expected for a clockwise cycle.
Eff = 1 - (273+45)/(273+120) = .19 = Work/Qin --> Qin = 3000 W/.19 = 15, 700 W and Qout = Qin - W = 12, 700 W. Note that we are really using power = Q/t in all cases. You can simply think of it as 3000 J of work every second, etc.