Chemistry Labs

Problem 2

Kinetic isotope effect (KIE) and zero-point vibrational energy (ZPE). The harmonic oscillator model gives the vibrational frequency ν=12πkμ\nu = \dfrac{1}{2\pi}\sqrt{\dfrac{k}{\mu}}, where kk is the force constant and μ=m1m2m1+m2\mu = \dfrac{m_1 m_2}{m_1 + m_2} is the reduced mass. Vibrational energies are En=(n+12)hνE_n = (n + \tfrac{1}{2})h\nu (n=0,1,2,…n = 0, 1, 2, \dots), and the zero-point energy is ZPE=12hν\text{ZPE} = \tfrac{1}{2}h\nu. (a) Calculate the reduced masses μCH\mu_{\ce{CH}} and μCD\mu_{\ce{CD}} in atomic mass units (u), taking m(C)=12.00m(\ce{C}) = 12.00 u, m(H)=1.008m(\ce{H}) = 1.008 u, and m(D)=2.014m(\ce{D}) = 2.014 u. (b) Given kCH=kCDk_{\ce{CH}} = k_{\ce{CD}} and the C−H\ce{C-H} stretching wavenumber ν~CH=2900 cm−1\tilde{\nu}_{\ce{CH}} = 2900\ \text{cm}^{-1}, calculate the C−D\ce{C-D} stretching wavenumber ν~CD\tilde{\nu}_{\ce{CD}} (cm−1^{-1}). (c) Calculate ZPECH\text{ZPE}_{\ce{CH}} and ZPECD\text{ZPE}_{\ce{CD}} in kJ mol−1^{-1}. (d) Calculate the difference in bond dissociation energies ΔBDE=BDECD−BDECH\Delta \text{BDE} = \text{BDE}_{\ce{CD}} - \text{BDE}_{\ce{CH}} (kJ mol−1^{-1}). (e) Assuming Ea≈BDEE_a \approx \text{BDE} and identical Arrhenius pre-exponential factors, calculate the theoretical primary KIE kCH/kCDk_{\ce{CH}}/k_{\ce{CD}} at 25 ∘C25\ ^{\circ}\text{C}. (f) In the chromic acid oxidation of diphenylmethanol, measured first-order rate constants are kCH=0.012 min−1k_{\ce{CH}} = 0.012\ \text{min}^{-1} and kCD=0.0018 min−1k_{\ce{CD}} = 0.0018\ \text{min}^{-1}. Compare this experimental ratio with the theoretical value and determine whether C−H\ce{C-H} bond cleavage is rate-determining.
Step 1 of 6: Calculate reduced masses
μCH=12.00×1.00812.00+1.008=0.930 u;μCD=12.00×2.01412.00+2.014=1.725 u\mu_{\ce{CH}} = \dfrac{12.00 \times 1.008}{12.00 + 1.008} = 0.930\ \text{u};\quad \mu_{\ce{CD}} = \dfrac{12.00 \times 2.014}{12.00 + 2.014} = 1.725\ \text{u}
Analysis

Applying μ=m1m2/(m1+m2)\mu = m_1m_2/(m_1+m_2) gives μCH=0.9299\mu_{\ce{CH}} = 0.9299 u and μCD=1.7246\mu_{\ce{CD}} = 1.7246 u (taking mD≈2mHm_D \approx 2m_H). Deuterium nearly doubles the reduced mass of the vibrating diatomic oscillator.