1 أحمد سعيد شلبي قسم الكيمياء كليه العلوم جامعه بنها امتحان ثالثه كيمياء خاصه.د.أ ميكانيكا احصائيه رابعه تخلف ثالثة Prof.Dr. Ahmad S. Shalabi ___________________________________________________________ Benha University 3rd year Students Date : 62-26-2011 Faculty of Science Special Chemistry Time : 3 hours Chemistry Department Staistical Mechanics ___________________________________________________________ Statistcal Thermodynamics ___________________________________________________________ 1- Based on the principle of equipartition of energy, write the values of the translational Et , rotational Er ,and vibrational Ev energies in terms of the gas constant (R). 2- Compare between the third law of thermodynamics and statistical entropies clarifying the different types of discrepant behavior. 3- Calculate the translational partition function for 1 mole of oxygen at 1 atm. pressure at 25 oC , assuming the gas to behave ideally. [Avogadro number : N=6.023 x 1023 - π= 3.2422 - k= 1.38 x 10 -16 R= 82.06 - h= 6.624 x 10 -27] . __________________________________________________________ GOOD LUCK 2 أحمد سعيد شلبي قسم الكيمياء كليه العلوم جامعه بنها امتحان ثالثه كيمياء خاصه.د.أ ميكانيكا احصائيه رابعه تخلف ثالثة Prof.Dr. Ahmad S. Shalabi ____________________________________________________________________ Benha University 3rd year Students Date : 26-12-2011 Faculty of Science Special Chemistry Time : 3 hours Chemistry Department Staistical Mechanics _____________________________________________________________________ Model Answers ___________________________________________________________________ 1. According to the principle of equipartition of energy of energy, each kind of energy of a molecule that can be expressed in the general form ax2 contribute an amount of RT to the average energy of one mole. The translational kinetic energy of a molecule is m/2 (x2 + y2 + z2) x , y, z : the components of velocity in the directions at right angles. momentum Px=mx. , and so the energy is given by 1/2m ( P2x + P2y + P2z ) thus, consisting of three quadratic terms. Consequently, . The translational energy is 3 x (1/2) x RT = RT 3 . The rotational energy of a molecule, assumed to be of constant dimensions, is proportional to the square of the angular momentum, so that rotation is represented by one quadratic or square terms and contributes 1 x (1/2) x RT = RT per mol The rotational energy of a diatomic or linear molecule, that exhibits rotations about two axes contributes 2 x (1/2) x RT = RT per mol The rotational energy of a non linear molecule, that exhibits rotations about three axes contributes 3 x (1/2) x RT = RT per mol . A non linear molecule containing (n) atoms have (3n-6) modes of vibrations, so that the vibrational energy contributes (3n-6)RT per mol A linear molecule containing (n) atoms have (3n-5) modes of vibrations, so that the vibrational energy contributes (3n-5)RT per mol 4 2. . Third Law ( thermal ) entropy Obtained from heat capacity measurements. It is zero at absolute temperature i.e perfect solid. . Statistical (standard) entropy Obtained from Boltzman-Planck equation i.e the combined rotational and vibrational partition functions Qr and Qv . Both types of entropies are in agreement. However some discrepancies occur for : CO, NO, NNO, H, D, H2O, and CH3-CH3 ( internal rotation). The various types of discrepant behavior will now be discussed: o Random Orientation in the Solid For CO, NO, and NNO . The third law considers one arrangement for solids CO CO NO NO NNO NNO 5 so that there is similarity between the two ends, and the probability of state is 1 so, S = R ln 1 = 0 This is not the case for randomly oriented solids, i.e it is not correct to take the entropy as zero. . Statistical mechanics considers two arrangements for solids CO OC NO ON NNO ONN so that there is no similarity between the two ends, and the probability of state is 2 so, S = R ln 2 ≠ 0 This is the case for randomly oriented solids, i.e it is correct to take the entropy as non zero. The same situation occurs for H2O : The third law considers ice as a perfect solid with zero entropy. While, in fact, there is a distribution of H bonds in ice crystal and the solid is not perfect so that entropy is not zero as predicted by statistical mechanics 6 3. Qt = (2πmKT)3/2 . V h3 = (2πmKT)3/2 . RT h3 P since Qt is dimensionless, the numerator and denominator must be expressed in the same units m,k,h in c.g.s, p in atm., R in cc.atm.deg.-1 mol.-1 m = M.W = 32_____ = 5.313 x 10-23 g N 6.023 x 1023 Qt=[2x 3.1414 x(5.313x10-23)x(1.38x10-16)x 298.2]3/2 . 82.06x298.2 [6.624x10-27]3 1 = 4.28x1030