Challenge: A Different Approach to Calculating Equilibrium Constants
In this challenge we are going to calculate the equilibrium constant for the reaction: \[Na_{2} (g) <-> 2 Na (g)\] At 1500 K we have got the following spectroscopic data: The dissociation energy D0 equals 70.4 kJ/mol The rotational constant B_Na2 equals 0,1547 cm^-1 The vibrational constant v_Na2 equals 159,2 cm^-1 In addition to that sodium is 2 times degenerated in the ground state.
Hint to solve the problem: Rewrite Gibbs' free energy so it depends of the molecular partition function and write up the contributions to the molecular partition function for Na and Na2. We assume at 1500 K that Na and Na2 acts as a ideal gas.
Good luck :)
Shouldn't that be Na* Where * means an off electron
As I have read this eq. : \(Na_2 <-> 2Na*\)
Actually, I was trying for Na* only.......
As I haven't wrote a charge I found it unnecessary to show it contains a single electron.
Thanks
Challenge questions shouldn't be anything higher than thermodynamics. Or o-chem.
It is thermodynamics. :)
But I sure like to post the solution if people like.
This challenge actually test your understanding for the equilibrium constant.
This is like university level statistical mechanics... not a chance anyone here would be able to solve without Googling.
First of all, \(K = \cfrac{(\cfrac{q^{0} Na}{N_A})^2 }{(\cfrac{q^{0} {Na}_2 }{N_A})} e^{-\beta \Delta \epsilon } \) where, \(\Delta \epsilon = -D_0 \) Total partition function for \(Na \cdot\) is, \(\mathsf{{q^0}_{Na} = {q^{\mathsf{Trans}}}_{Na} \times {q^{\mathsf{elec}}}_{Na} \\ \quad \quad \space = {2q^{\mathsf{Trans}}}_{Na} = 9780.54 * 10^{34} }\) Also, molar volume : \(\mathsf{V =\cfrac{RT}{P} } \) = \(0.12308 m^3 \) \(\mathsf{Since ~ P = 1.01325 * 10^{5} ~ Pa ; ~ T = 15000 K }\) Transitional partition function for \(Na \cdot\) is ; \(\mathsf{{q^{\mathsf{Trans}}}_{Na} = \cfrac{V \times (2\pi m_{Na} k T )^{\cfrac{3}{2}} }{h^3} }\) \(\quad \quad \quad \mathsf{= \cfrac{0.12308 \times [2\times 3.14 \times \cfrac{23.5}{6.023 \times 10^{23} } \times 1.38 \times 10^{-23} \times 1500]^\cfrac{3}{2} }{(6.6 \times 10^{-34})^{3} }}\) \(\mathsf{Since ~ {Na}_2 ~ has ~ no ~ unpaired ~ e^{-} . \\ Therefore ~ electronic ~ partition ~ function ~ = 1}\) \(\mathsf{Therefore ~ Total ~ paritition ~ function ~ for ~ {Na}_2 ~ molecule ~ is, \\ {q^0}_{{Na}_2} = {q^{trans}} _ {Na_2} {q^{rot}} _ {Na_2} {q^{vib}} _ {Na_2} {q^{elec} }_ {Na_2} \\ \quad = {q^{trans}} _ {Na_2} {q^{rot}} _ {Na_2} {q^{vib}} _ {Na_2} }\) Since, \(\mathsf{\cfrac{{q^{trans}}_{Na_2}}{{q^{trans}}_{Na} } = (\cfrac{m_{Na_2} }{m_{Na}})^\cfrac{3}{2} = 2^\cfrac{3}{2} }\) Therefore, \(\mathsf{{q^{trans}}_{Na_2} = 2^\cfrac{3}{2} \times {q^{trans}}_{Na} = 13829.694 \times 10^{34} }\) Also, \(\mathsf{{q^{rot}}_{Na_2} = \cfrac{T}{2\theta _R} \\ \quad \quad = \cfrac{kT}{2ncB} \\ \quad \quad = \cfrac{1.38 \times 10^{-23} \times 1500}{2 \times 6.6 \times 10^{-34} \times 3 \times 10^8 \times 0.1547 \times 10^2 } \\ \quad \quad = 3378.974 }\) Also, \(\mathsf{{q^{vib}}_{Na_2} = \cfrac{1}{1-e^{\cfrac{-nc\nu }{kT}}}}\) \(\mathsf{\quad \quad = \cfrac{1}{1-e^{\cfrac{-6.6 \times 10^{-34} \times 3 \times 10^{8} \times 1592 \times 10^2 }{1.38 \times 10^{-23} \times 1500}}}}\) \(\mathsf{ = 1.278944 } \) Put all the values and solve : \(\mathsf{K = \cfrac{({q^0}_{Na_2} )^2}{N_A ({q^0}_{Na_2} )} \times e^{\cfrac{70400}{RT}}}\) \(\mathsf{K = 751.916599 \times 10^{10}}\)
I never tried such questions in past. This is my first time, so pardon my mistakes (if there are).
Well written mathslover i got to say I'm impressed, however your expression for the equilibrium I'm unsure how you got to: Lets observe the following expression for the equilibrium constant: \[\ln(K)=-\frac{ \Delta _{r}G ^{\Theta} }{ RT }\] For a ideal gas you can show that: \[G _{m}-G _{m}(0)=-RT \ln(\frac{ q }{ N_{A} })\] But the standard reaction Gibbs free energy is defined as: \[\Delta _{r}G ^{\Theta}=\sum_{J}^{}v _{j}G_{m,j}^{\Theta}\] Then it follows that we have to use standard molecular Gibbs energies of each component j: \[G_{m,j}^{\Theta}=G _{m,j}^{\Theta}(0)-RT \ln(\frac{ q _{m,j}^{\Theta} }{ N_{A} })\] Here is q_m,j,theta the standard molecular partition function of the component j. So the relationship between the standard reaction Gibbs free energy and the standard molecular partition function: \[\Delta _{r}G ^{\Theta}=\sum_{J}^{}v _{J}G _{m,J}^{\Theta}=\sum_{J}^{}v _{J}G _{m,J}^{\Theta}(0)-RT \sum_{J}^{}v _{j}\ln(\frac{ q _{m,J}^{\Theta} }{ N _{A} })\] But for a ideal gas it follow at T=0 K that G(0)=A(0)=U(0) and thereby: \[\sum_{J}^{}v _{J}G _{m,J}^{\Theta}(0)=\sum_{J}^{}v _{J}U _{m,J}^{\Theta}(0)=\Delta _{r}U ^{\Theta}(0)\] But is different from the internal energy at T=0 and therefor is nothing else than the difference in energies in the lowest state of all components: \[\Delta _{r}U ^{\Theta}(0)=N _{A}\sum_{J}^{}v _{J} \epsilon _{0, J} \equiv \Delta _{r}E _{0}\] Put everything together so we for the reaction Gibbs free energy get: \[\Delta _{r}G ^{\Theta}=\Delta _{r}E _{0}-RT \sum_{J}^{}v _{J} \ln(\frac{ q _{m,J}^{\Theta} }{ N _{A} })\] Compair with out first expression for the equilibrium constant and we get the equation: \[K=\exp(-\frac{ \Delta _{r}E _{0} }{ RT }+\sum_{J}^{}v _{J}\ln(\frac{ q _{m,J}^{\Theta} }{ N _{A} }))\] We can rewrite that using a power calculation rule (the a^(x+y)=a^x*b^y): \[K=\exp(-\frac{ \Delta _{r}E _{0} }{ RT })\prod_{J}^{}\left( \frac{ q _{m,J}^{\Theta} }{ N _{A} } \right)^{v _{J}}\] So think you used the the Avogadro constant one time to much.
You frightened me , I got this equation in a formula bank and I used it .
This is out of my syllabus, in 10th standard, I never learnt such things, so sorry that I will not be able to explain you that formula. But thanks for the medal :)
I think you did a awesome try! :D
Thanks for the quest.
The molecular partition functions:
Why Na is two times degenerated is due to the unpaired electron can have spin up or down if I forgot to tell that.
And the results: :)
But I'm a undergraduate @abb0t :( on his first year :(
Ok.
how the hell are you a first year undergraduate in statistical mechanics?
It's like asking how to fly a plane even though you haven't learned to drive a car yet
@oldrin.bataku I can show you this is what the course description say: "After the course, students should be able to: • define and explain the Laws of Thermodynamics • define and apply the thermodynamic variables T and p, the statistical thermodynamic partition functions q and Q and the thermodynamic functions U, S, H, A and G and their partial derivatives and the electrochemical potential E. • calculate the activity of an ion in a dilute electrolyte solution by using the Debye-Hückel expression. • specify the conditions for spontaneous processes, and explain the work (on the environment) and heat generation by their course • specify the condition for a chemical reaction is spontaneous and derive eqilibrium • apply the thermodynamic functions to describe the phase equilibria and phase transitions in physico-chemical systems • apply the thermodynamic functions of mixtures and chemical reactions • apply the thermodynamic functions of the electrolyte and electrochemical reactions • write the redox process of a component of an electrochemical reaction and its electrochemical potential using the Nernst's law • apply the thermodynamic functions of biochemical processes: membrane potentials and kolloidosmotisk pressure • apply the statistical thermodynamic partition functions q and Q to calculate the thermodynamic functions U, S, H, A, G and equilibrium constant of phase equilibria or chemical reactions • write the expression of a molecule's speed and the mean free path length in a gas • define and explain the spontaneous processes time courses, including chemical kinetics • Explain in simple enzyme-controlled reactions"
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