Chemistry Labs

Problem 1

Particles in a box: polyenes. In quantum mechanics, the movement of π electrons along a neutral chain of conjugated carbon atoms may be modeled using the 'particle in a box' method. The energy of the π electrons is En=n2h28mL2E_n = \dfrac{n^2 h^2}{8 m L^2}, where nn is the quantum number (n=1,2,3,…n = 1, 2, 3, \dots), hh is Planck's constant, mm is the mass of the electron, and LL is the length of the box, approximated by L=(k+2)×1.40 A˚L = (k + 2) \times 1.40\ \text{Å} (kk being the number of conjugated double bonds along the carbon chain). A photon of wavelength λ\lambda can promote a π electron from the HOMO to the LUMO. A semi-empirical formula relates λ\lambda to kk: λ=B×(k+2)22k+1\lambda = B \times \dfrac{(k+2)^2}{2k+1} (Equation 1). (a) Using Equation 1 with B=65.01B = 65.01 nm, calculate λ\lambda for octatetraene, CHX2=CH−CH=CH−CH=CH−CH=CHX2\ce{CH2=CH-CH=CH-CH=CH-CH=CH2}. (b) Derive Equation 1 from the particle-in-a-box expression and calculate the theoretical value BcalcB_{\text{calc}}. (c) Find the number of conjugated double bonds kk and give the structure of the polyene whose HOMO–LUMO excitation requires λ=600\lambda = 600 nm. (d) For that polyene, calculate the HOMO–LUMO energy difference ΔE\Delta E in kJ mol−1^{-1}.
Step 3 of 4: Solve for kk at λ=600\lambda = 600 nm
600=64.6×(k+2)22k+1⇒k2−14.58k+⋯=0⇒k1=14.92,  k2=−0.36⇒k=15600 = 64.6\times\dfrac{(k+2)^2}{2k+1} \Rightarrow k^2 - 14.58k + \dots = 0 \Rightarrow k_1 = 14.92,\; k_2 = -0.36 \Rightarrow k = 15
Analysis

Setting λ=600\lambda = 600 nm in the derived equation gives a quadratic in kk with roots k1=14.92k_1 = 14.92 and k2=−0.36k_2 = -0.36; only the positive integer solution is physical, so k=15k = 15 and the polyene is CHX2=CH−(CH=CH)X13−CH=CHX2\ce{CH2=CH-(CH=CH)13-CH=CH2}.

Common pitfall. Keep the negative root k2=−0.36k_2 = -0.36 out of the answer — a polyene cannot have a negative or non-integer number of double bonds.