How do you calculate the average kinetic energy of the CH_4CH4 molecules in a sample of CH_4CH4 gas at 253 K and at 545 K?
1 Answer
The average kinetic energy
Suppose
For methane this is a decent approximation that omits vibrational degrees of freedom; I'll talk about it at the bottom of the answer.
For the equipartition theorem, we have:
\mathbf(K_"avg" = N/2nRT)Kavg=N2nRT where:
NN is the number of degrees of freedom.nn is the number of\mathbf("mol")mol s.RR is the universal gas constant,"8.314472 J/mol"cdot"K"8.314472 J/mol⋅K .TT is the temperature in"K"K .
NOTE: If you include the vibrational contribution to the degrees of freedom according to the equipartition theorem (
Given
Thus, we have
color(blue)(K_"1,avg") = 6/2RT_1K1,avg=62RT1
= 3*8.314472*253=3⋅8.314472⋅253
= "6310.68 J" ~~ color(blue)(6.31xx10^3 "J")=6310.68 J≈6.31×103J
color(blue)(K_"2,avg") = 6/2RT_2K2,avg=62RT2
= 6/2*8.314472*545=62⋅8.314472⋅545
= "13594.2 J" ~~ color(blue)(1.36xx10^4 "J")=13594.2 J≈1.36×104J rounded to three sig figs.
NOTE: This corresponds to an estimated constant-volume molar heat capacity of
This is a decent approximation but could be better because methane has four vibrational modes in its IR spectrum (
These contribute a total of
barC_"V,tot" = barC_"V,trans" + barC_"V,rot" + barC_"V,vib"¯¯¯CV,tot=¯¯¯CV,trans+¯¯¯CV,rot+¯¯¯CV,vib
= 3/2R + 3/2R + 0.2823R=32R+32R+0.2823R
~~ color(blue)(3.2823R)≈3.2823R
whereas the equipartition theorem predicts:
barC_"V,tot" = barC_"V,trans" + barC_"V,rot" + barC_"V,vib"¯¯¯CV,tot=¯¯¯CV,trans+¯¯¯CV,rot+¯¯¯CV,vib
= 3/2R + 3/2R + stackrel("omit this for ideality")(overbrace(9R)
= color(red)(stackrel("'real'")(overbrace(12R)) , orcolor(red)(stackrel("ideal")(overbrace("3R")) which is fairly off from the true
barC_("V,tot") !
And just so you know I'm not making these numbers up, I got this information while doing a speed-of-sound in methane lab last year:
barC_(V_"vib") = Rsum_(i)^(3N-6) [g_i((theta_i)/T)^2 e^(-theta_i"/"T)/(1-e^(-theta_i"/"T))^2]
(from my lab handout)where:
R is the universal gas constant.g_i is the degeneracy of modei .E is doubly degenerate andT is triply degenerate (A is unique, sog_A = 1 ).N here is the number of atoms on"CH"_4 :5 .theta_i is the vibrational temperature in"K" of vibrational modei . Those are given in Table 1 below.T is temperature in"K" as usual.
And a summary of
The takeaway is that the statistical mechanics approach was the most accurate approach.