If #DeltaH_c^@# of solid benzoic acid at 27°C is -x kcal/mol, then #DeltaE_c^@# (in kcal/mol) is?
- -x + 0.9
- -x + 0.3
- -x - 0.9
- -x - 0.3
EDIT: In a bomb calorimeter.
- Truong-Son
- -x + 0.9
- -x + 0.3
- -x - 0.9
- -x - 0.3
EDIT: In a bomb calorimeter.
- Truong-Son
2 Answers
Explanation:
Combustion of 1 mol of benzoic acid
#"C"_6"H"_5"COOH"_"(s)" + 15/2"O"_"2(g)" -> "7CO"_("2(g)") + "3H"_2"O"_"(l)"#
#Δ"H"_"c"^0 = Δ"E"^0 + Δ"n"_"g" "RT"#
By definition, at constant temperature and pressure, the change in enthalpy is given by:
#DeltaH = DeltaE + Delta(PV) = DeltaE + PDeltaV#
#= DeltaE + Deltan cdot RT# where
#DeltaE# is the change in internal energy,#Deltan# is the change in mols of ideal gas, and#R# and#T# are known from the ideal gas law.
So then, for a combustion, the change in internal energy is given by:
#DeltaE_c^@ = DeltaH_c^@ - Deltan_"gas" cdot RT#
For the combustion of benzoic acid in a bomb calorimeter CLOSED to the atmosphere, we have a constant-volume vessel that condenses the water vapor back to a liquid from the initial non-equilibrium gaseous state:
#"C"_6"H"_5"COOH"(s) + 15/2"O"_2(g) -> 7"CO"_2(g) + 3"H"_2"O"(l)#
Of course, if you did this open to the atmosphere, you would get
#Deltan_"gas" = 7 - 15/2 = -"0.5 mols ideal gas"#
If this was done open to the atmosphere (which is a condition that was aptly unstated in the problem!), then
Hence, in a bomb calorimeter,
#DeltaE_c^@ = overbrace(-x " kcal/mol")^(DeltaH_c^@)#
#- [overbrace(-0.5 cancel"mols ideal gas")^(Deltan_"gas") xx overbrace(8.314472 cancel"J""/mol"cdotcancel"K" xx cancel("1 cal")/(4.184 cancel"J") xx "1 kcal"/(1000 cancel"cal"))^(R) xx overbrace((27 + 273.15 cancel"K"))^(T)]#
#= -x + "0.298 kcal/mol"#
And from the given answers, we are closest to
#color(blue)(DeltaE_c^@ ~~ -x + "0.3 kcal/mol")# .