1. A system does 3 J of work on the surroundings, and 12 J of work are added to the system. What is the energy change of the system? 9 J What is the energy change of the surroundings? -9 J
2. A quantity of 0.850 mol of an ideal gas initially at a pressure of 15.0 atm and 300K is allowed to expand isothermally until its final pressure is 1.00 atm. Calculate the value of the work done if the expansion is carried out (a) against a vaccum, (b) against a constant external pressure of 1.00 atm, and (c) reversibly – use the equation wrev=-nRT*ln(P1/P2).
a.) w=-PextDV, here Pext = 0, so w=0
b.) Pext=1.00 atm. Find initial and final volumes using the ideal gas law:
V1=nRT/P1; V2=nRT/P2; w=-PextDV, where Pext is equal to P2
DV= V2-V1 = nRT({1/P2}-{1/P1})
Therefore, w=-nRTP2({1/P2}-{1/P1}) = -19.5 L*atm = -1.98*103 J
c.) for an isothermal, reversible process, we use the following equation for work:
wrev=-nRT*ln(V2/V1)=-nRT*ln(P2/P1) = -5.74*103 J
3. Calculate the values of DE and DH for the heating of 55.40 g of xenon from 300 K to 400 K. Assume ideal-gas behavior and that the heat capacities at constant volume and constant pressure are independent of temperature.
Xenon is a monatomic “ideal” gas, so Cv=3/2*R and Cp=5/2*R (always true for ideal monoatomic gases). We have the two following equations (always true):
DE=nCvDT = 526J; DH=nCpDT = 877 J
DE=nCvDT = 526J; DH=nCpDT = 877 J
4. Calculate the entropy change when 2.0 mol of an ideal gas are allowed to expand isothermally from an initial volume of 1.5 L to 2.4 L.
DS=nR*ln(V2/V1) = 7.8 J/K
5. A quantity of 0.50 mol of an ideal gas at 20oC expands isothermally against a pressure of 2.0 atm from 1.0 L to 5.0 L. Calculate DSsys, DSsurr, and DSuniv.
Use the ideal gas law to find initial pressure = 12 atm. Use the equation:
DSsys = nR*ln(V2/V1) = 6.7 J/K
DSsurr = qsurr/T; DE=0 since DT=0 (it is an isothermal process). Therefore, w=-q. We can calculate w=-PDV, and qsys=-qsurr, so qsurr=w. We get DSsurr = -2.8 J/K
DSuniv=DSsys+DSsurr=3.9J/K
DSuniv=DSsys+DSsurr=3.9J/K
6. Supercooled water is liquid water that has been cooled below its normal freezing point. This state is thermodynamically unstable and tends to freeze into ice spontaneously. Suppose we have 2.0 mol of supercooled water turning to ice at -10oC and 1.0 atm. Calculate DSsys, DSsurr, and DSuniv for this process (set up a thermodynamic cycle). Cp water = 75.3 J/K*mol and Cp ice = 37.7 J/K*mol; the molar heat of fusion of water is 6.01 kJ/mol. (DSfus=n*DHfus/T, qsurr=n*DHfus)
Step 1: Water at -10 à Water at 0:
DS = nCp*ln(Tf/Ti) = 5.6 J/K
Step 2: Water freezes at 0:
DSfus=DHfus/T = -44.0 J/K
Step 3: Ice at 0 à Ice at -10:
DS = nCp*ln(Tf/Ti) = -2.8 J/K
Therefore, DStot=DSsys =5.6 J/K - 44.0 J/K - 2.8 J/K = -41.2 J/K
To find DSsurr, we must find q for each step, add those numbers together and plug into the equation DSsurr = qrev/T.
Step 1: qsurr=-nCPDT = -1.5 kJ
Step 2: qsurr=n*DHfus = 12 kJ
Step 3: qsurr=-nCpDT = 754 J
Step 2: qsurr=n*DHfus = 12 kJ
Step 3: qsurr=-nCpDT = 754 J
qsurr(tot) = 11 kJ, DSsurr=41.8 J/K
DSuniv = DSsys + DSsurr = 0.6 J/K
7. A 0.590 mol sample of an ideal gas initially at 300 K and 1.50 bar is compressed isothermally to a final pressure of 6.90 bar. Calculate the change in Gibbs energy for this process.
For an ideal gas, DG = nRT*ln(P2/P1) = 2.23 kJ
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