In: Chemistry
A sample containing 321.5 g of nitrogen gas is expanded isothermally at T=298 K from 1.023dm^3 to 57.28dm^3. Calculate q, w, delta U and delta H for four processes assuming N^2 behaves ideally:
(a.) in a vacuum
(b.) against a constant external pressure equal to the final pressure of the sample
(c.) reversibly
(d.) adiabatically (non-isothermal)
a) In the case of expansion of any gas work is done by the system.
Now we know that
w = -pextV = -pext (Vf - Vi)
where p external = external pressure ofthe system = 0
Thus the work done by the system will be: w = 0( 57.28dm^3 - 1.023dm^3)
= 0
Also q (heat) absorbed is the cosequence of gaining temperature.But gere it is at constant temperature.
q=-w
so q=0 hence no heat is absorbed.
As the process is isothermal, the change in internal energy=0
and deltaH= deltaU -p V
hence H = zero.
b) Given the amount of N2 is---------------321.5g = 321.5/28 moles
= 11.5 moles
T= 298K
Vi = 1.023dm^3 = 1.023litres
We know the ideal gas equation: PV = nRT
Therefore Pi = nRT/Vi
= (11.5* 0.0821 lir.atm/mol K * 298)/1.023 lit
= 275 atm
We know that according to Boyles law:
P1V1=P2V2
therefore final pressure P2= P1V1/V2
= (275 atm * 1.023 lit)/ 57.28lit
= 4.91 atm (THIS IS THE FINAL EXTERNAL PRESSURE)
Pext = 4.91 atm
Vf = 57.28lit
Vi=1.023 lit
Hence w= - Pext(Vf-Vi)
= - 4.91atm(57.28-1.023)L
= -276.2 atm L
In isothermal expansion: q=-w
therefore q= 276.2 atm.L
U = 0 and H = U + w
= -276.2 atm L
c) Reversible isothermal expansion : Then work done = -2.303 nRT log Vf/Vi
= - 2.303 * 11.5moles * 0.0821 L atm/mol K* 298K * log (57.28/1.023)
= - 1132.7 L atm
q= -w
= 1132.7 L atm
delta U = 0 (isothermal)
delta H = delta + w
= -1132.7 atm.L
d)Adiabatic process q= 0
Hence the change in internal energy = work done
We know that for an ideal gas:
T1V1-1= T2 V2-1
T2 = T1 (V1/V2)-1 = 298 * (1.023/57.28)1.4-1
= -208.4K
Hence work done= nR(T2-T1)/1-
= 11.5 * 0.0821 ( -208.4-298)/ (1-1.4) since gamma value for a diatomic gas is 1.40
= 1195.3 L atm
Delta U = 1195.3 L atm