To write and balance the reaction equation, we have to first know what the molecular formula
of the CxHyOz is. So this is a deja vu
empirical/molecular formula problem masquerading as an ideal gas one.
n(CxHyOz) = PV/RT = 1 atm (10.0 L) / [ 0.08206 atm L/mol K (473 K) ] = 0.258 moles which makes the molecular weight 16.0 g/0.258 mol = 62.1 g/mol
n(C) = 22.7 g CO2 × 1 mol CO2/44.01 g CO2 = 0.516 mol C
wt(C+H) = 12.01 g/mol × 0.516 mol + 1.008 g/mol × 1.543 mol = 7.75 g n(O) = 8.25 g / 16.00 g/mol = 0.515 mol O CxHyOz = C0.516H1.543O0.515 = CH3O for an empirical formula. But it would have an empirical formula weight of 12.01+3(1.008)+16.00 = 31.05 g/mol, half the known molecular weight. So the molecular formula must be C2H6O2, probably ethanediol, HOCH2CH2OH, but we can't be sure of that since there's more than one isomer of that combination of elements.
|
welec = DG° =
2 DGf°[H2O(liq)] = 2(-237 kJ/mol)
= - 474 kJ/mol, the negative sign implying the battery does work.
wPV = - PDV = - RT Dngas = - 8.314 J/mol K (298 K) (-3) = + 7.43 kJ/mol, the plus sign implying that the atmosphere does work on the system (by compressing the gases flat). |
Looking at the reaction equation on page 851,
we see that the electrolysis produces not only the expected gaseous products but also a (briefly) separated quartet of (H+ , OH - ) pairs. The latter's recombination to form water gives up four Heats of Neutralization (which you can calculate from Appendix 4 if you are of a mind to) which heats up the solution, wasting exactly the difference in the energies which give rise to that extra voltage. |
DE = (0.0592 V / n) log(PO2) = (¼)(0.0592 V) log(0.21) = - 0.01 V = - 10 mV |
DE = (0.0592 V / n) log(PO2 × P2H2) = (¼)(0.0592 V) log(353) = + 0.069 V = + 69 mV |
DHvap / DHfus
= 40.7 kJ/mol steam / 6.02 kJ/mol ice = 6.76 mol ice/mol steam.
But that leaves the steam at 100°C. We have to cool it to 0°C.
CP = 4.197 J/g°C × 18.02 g/mol H2O = 75.63 J/mol°C
Total moles of ice = 6.76 + 1.26 = 8.02 moles of ice to condense 1 mol steam to 0°C. |
The toothpick starts moving in the direction of its non-soapy end. |
The soap destroys water's surface tension and so reduces its grip on the soapy end. |
Eventually, the soap spreads, reducing the tension all over the water's surface uniformly. No direction is then favored. |
Imagine an overall second order elementary gas phase reaction A + B at 1 atm total pressure at
25°C. Imagine that a solid catalyst captures multilayers of both molecules at liquid-like
concentrations, say 10 M each. By what factor is the reaction rate improved through this
"concentration" effect, ignoring any other kind of surface catalytic activity?
Rate = k2 [A] [B] = k [A]2 since [A] = [B]
Ratecondensed / Rategaseous = [A]2condensed / [A]2gaseous [A]gas = nA / V = PA / RT = ½ atm / [0.08206 atm L/mol K (298 K)] = 0.0204 mol/L Ratecondensed / Rategaseous = (10 M)2 / (0.0204 M)2 = 2.4×105 (!) |
It maintains that the dense salt solution at the bottom of the tank cannot boil at 107°C since its boiling point is "much higher than 100°C." With the tools at our command, we can test that prediction.
In 1 kg of solution there are 270 g NaCl and 730 g H2O. We'd have to scale the
water's weight up by (1000/730)=1.37 to make a kg of solvent, and the solution that
had that much solvent would, perforce, contain 1.37×270 = 370 g NaCl.
molality NaCl = 370 g NaCl ( 1 mol NaCl / 58.5 g NaCl ) = 6.3 m Assuming it dissociates 100% (not bloody likely), there'd be 12.6 m ions in solution, and the boiling point elevation would be: DT = Kb mions = 0.51°C kg/mol (12.6 mol/kg) = 6.4°C Actually it's less since the vant Hoff factor for NaCl isn't as much as 2 at such concentrations. Even at 1% of that concentration, i = 1.9 for NaCl (Table 11.6). So boiling point elevation alone cannot account for unboiled salt water at 107°C. |
Layer | Thickness (m) | % by wt NaCl | Est. Density (g/cc) | DP (atm) |
Convective | 0.5 m | 2% | ||
Non-convective | 1.5 m | 15% | ||
Bottom | 1.0 m | 27% | ||
Extra pressure due to weight of all the water (atm): |
We've already seen in part (a) that 1000 kg of bottom water (I like the sound of that)
carries an additional 370 g of salt. So if it still occupies only a liter (unlikely), the
density of bottom water would be 1370 g/L or 1.37 g/mL, 37% heavier than pure water.
The pressure that the bottom layer exerts on the pond floor is that which an equivalent height of mercury would exert scaled by the difference in their densities. DP3 = (1 atm/0.76 m Hg)(1.0 m)(1.37 g/mL H2O / 13.6 g/mL Hg) = 0.133 atm The intermediate layer is only 150 g salt to 850 g water; so 1000 g water contains 176 g of salt in a liter (ho ho ho) making the density 1.176 g/mL. It's pressure differential is: DP2 = (1/0.76)(1.5)(1.176/13.6) = 0.17 atm And the top layer similarly: 20 g salt in 980 g water means 1020 g/L or 1.020 g/mL hence DP1 = (1/0.76)(0.5)(1.020/13.6) = 0.05 atm and the table becomes:
Now we relate pressure to boiling point temperature by the Clausius-Clapeyron equation: P = 1 atm e-(DHvap/R) [(1/T) - (1/Tnbp)] where "nbp" is the normal boiling point. We know we want P = 1.35 atm so we have to rearrange C-C to find the corresponding T:
T = 1 / [(1/Tnbp) - (R/DHvap)ln(P in atm)]
DT = 382 - 373 = 9°C |
Tbottom = 100°C + 6°C + 9°C = 115°C |
k1 = ln(2) / t½ = 0.693 / 5700 yr =
1.22×10-4 yr-1
[14C] = [14C]0 e-k1t
|
The situation when Dngas = 0 is less obvious. What sort of differences between reactants and products can be exploited to guess the sign of DS then?
We can look for complexity changes. If few large molecules become several small ones,
DS increases.
If there are the same number of molecules in reactants and products but some reactant molecules are solids while products are all in solution, DS increases. If all are in the same phase and there are the same number of reactant and product molecules but products represent more mixed atoms (e.g., H2 and F2 reacting to make 2 HF), DS increases. |
k1 = A e-Eact/RT1
k2 = A e-Eact/RT2 k2/k1 = e(-Eact/R)[(1/T2) - (1/T1)] ln(k2/k1) = (-Eact/R) [ (1/T2) - (1/T1) ]
T2 = 1 / [ (1/T1) - (R/Eact)ln(k2/k1) ]
|
Not a problem: PbSO4(s)
Pb2+(aq) + SO42 - (aq)
DGsp° = - RT ln Ksp = - 8.314 J/mol K (298 K) ln (1.3×10-8) = 45.0 kJ/mol But DGsp° = DGf°[Pb2+(aq)] + DGf°[SO42 - (aq)] - DGf°[PbSO4(s)] or
DGf°[Pb2+(aq)] =
DGsp° -
DGf°[SO42 - (aq)] +
DGf°[PbSO4(s)]
|
Comments to Chris Parr | Return to CHM 1316 HomePage | Last modified 5 May 1999. |