13 Pages

fes11

Course: CHEM 444, Fall 2011
School: Delaware
Rating:
 
 
 
 
 

Word Count: 3296

Document Preview

Section NAME: Circle Number: 10 11 80 CHEMISTRY 444, SPRING, 2011(11S) Final Examination, May 25, 2011 81 Answer each question in the space provided; use back of page if extra space is needed. Answer questions so the grader can READILY understand your work; only work on the exam sheet will be considered. Write answers, where appropriate, with reasonable numbers of significant figures. You may use only the...

Register Now

Unformatted Document Excerpt

Coursehero >> Delaware >> Delaware >> CHEM 444

Course Hero has millions of student submitted documents similar to the one
below including study guides, practice problems, reference materials, practice exams, textbook help and tutor support.

Course Hero has millions of student submitted documents similar to the one below including study guides, practice problems, reference materials, practice exams, textbook help and tutor support.
Section NAME: Circle Number: 10 11 80 CHEMISTRY 444, SPRING, 2011(11S) Final Examination, May 25, 2011 81 Answer each question in the space provided; use back of page if extra space is needed. Answer questions so the grader can READILY understand your work; only work on the exam sheet will be considered. Write answers, where appropriate, with reasonable numbers of significant figures. You may use only the "Student Handbook," a calculator, and a straight edge. 1. (10 points) (a) The critical temperature of CO2 is 31.1C. Considering CO2 to be an ideal gas, what DO NOT WRITE is the mean free path at a pressure of 1 bar and this temperature? IN THIS SPACE Using an equation in the handbook, one must find the molecular diameter and the number density. For an ideal gas, the number density is (1 105 )(6.02211415 1023 ) = = = 2.3806 1025 3 (8.3144349 1 )(304.25 ) = (0.4328 109 )2 = 5.885 1019 2 p. 1________/10 p. 2________/10 p. 3________/10 p. 4________/15 The Lennard-Jones diameter of CO2 is 0.4328 nm, which gives a collision cross-section of 1 1 Substitution into the equation for the mean free path gives = 2 = 2(5.885 1019 2 )(2.3806 1025 3 ) p. 5________/10 p. 6________/10 = 5.0472 10 8 p. 7________/15 p. 8________/10 p. 9________/15 p. 10_______/10 p. 11_______/10 p. 12_______/10 (b) The critical pressure of CO2 is 73.9 bar. Again, if one assumes that CO2 under these conditions ============= can be treated as an ideal gas (a questionable assumption), what is the predicted mean free path at p. 13_______/10 the critical point? (Extra credit) ============= The only factor that changes in the calculation is the number density: TOTAL PTS 5 23 ) (out of 135) (73.9 10 )(6.02211415 10 = = (8.3144349 1 )(304.25 ) 1 Then, substitution in the equation yields = 2 = 2(5.885 1 1019 2 )(1.7593 This is only slightly larger than the diameter of the CO2 molecule. = 1.7593 1027 3 1027 3 ) = 6.8297 1010 NAME: CHEM 444, Final Exam, Spring, 2011, page 2 2. (10 points) The diffusion coefficient of the protein lysozyme (MW = 14.1 kg mol ) in dilute water solution is 0.10410 m -1 s at 25C. (a) How long will it take, on average, for the protein to diffuse an rms distance of 1 m under these conditions? -1 -9 2 For three-dimensional diffusion (which this has to be!), the rms distance travelled in some time is = 6 . Rearranging this equation gives the following equation for the time to travel an rms distance: (1 106 )2 2 = = = 1.60 103 6 6(0.104 109 2 1 ) (b) Assuming that the viscosity of this dilute solution is not affected by the presence of the protein, estimate the size of the protein (treated as roughly a sphere of radius r)? This assumption means that one should treat the solution as if it has the viscosity of water, which from the handbook is 8.937 millipoise at 25C. Then, one solves the Stokes-Einstein equation for the radius of the equivalent sphere: = 6 = 1.38065051023 1 (298.15 ) 6(8.937103 )(0.1 1 )(0.104109 2 1 ) = 2.350 109 Score for Page NAME: CHEM 444, Final Exam, Spring, 2011, page 3 3. (10 points) The interchange of forms for cyclohexane by the following process has been measured by NMR spectroscopy. [Anet, F. A. L.; Bourn, A. J. R. J. Am. Chem. Soc. 1967, 89, 760 768.] The rate constants, k, for the backward and forward processes are identical. The rate constants at various temperatures are given in the table. From these data, determine the activation energy for this process and the preexponential factor. -1 -1 k (s ) k (s ) Temperature (C) Temperature (C) -116.7 0.004 -81.8 4.00 -112.1 0.014 -77.9 6.40 -107.3 0.039 -61.4 64.00 -105.3 0.071 -42.4 566 -100.4 0.11 -34.4 1150 -96.9 0.27 -24.0 2490 8 One plots the natural logarithm of the rate constant versus 1/T, as shown in the adjacent graph. From the slope of the line, one finds the activation energy: 6 = . . = . = . 4 y = -5621.9x + 30.607 ln(k/s-1) 2 The intercept is related to the preexponential factor: 0 = (. ) = . -2 -4 -6 -8 0.003 0.004 0.005 0.006 0.007 1/T (1/K) Score for Page NAME: CHEM 444, Final Exam, Spring, 2011, page 4 4. (15 points) Given the following reaction mechanism, determine the rate expression for the production of HBr. (1) Br2 1 2 Br (2) Br +H 2 2 H + HBr (3) H + Br2 3 Br +HBr k k k (4) H + HBr 4 Br +H 2 k (5) 2 Br k 5 Br2 Solution: d [ HBr ] (I) = k 2 [ Br ][ H 2 ] + k 3 [ H ][ Br2 ] k 4 [ H ][ HBr ] dt d [ Br ] = 0 = 2k1 [ Br2 ] k 2 [ Br ][ H 2 ] + k 3 [ H ][ Br2 ] + k 4 [ H ][ HBr ] 2k 5 [ Br ]2 dt d [ H ] (III) = 0 = k 2 [ Br ][ H 2 ] k 3 [ H ][ Br2 ] k 4 [ H ][ HBr ] dt (II) Adding II and III gives: 0 = 2k1 [ Br2 ] 2k 5 [ Br]2 k [ Br ] = 1 [ Br2 ] k 5 1/ 2 (IV) Solving III for hydrogen radical gives: k1 1 / 2 1/ 2 k 2 ([ Br2 ]) [ H 2 ] k5 [H ] = k 3 [ Br2 ] + k 4 [ HBr] (V) Subtracting III from I (i.e., subtracting zero from I) gives: d [ HBr ] = 2k 3 [ H ][ Br2 ] dt (VI) Thus, the rate of production of HBr is: 1/ 2 k 1/ 2 k 2 1 ([ Br2 ]) [ H 2 ] k d [ HBr ] = 2k 3 [ Br2 ] 5 dt k 3 [ Br2 ] + k 4 [ HBr ] 1 2k 3 k 2 k1 / 2 k 51 / 2 ([ Br2 ]) [ H 2 ] [ HBr ] k3 + k4 [ Br2 ] 1/ 2 = Score for Page NAME: CHEM 444, Final Exam, Spring, 2011, page 5 5. (10 points) The decarboxylation of a -keto acid is catalyzed by a decarboxylase. The rate of the reaction is monitored by the production of CO2, which is produced by the decarboxylation with 1/1 stoichiometry. The initial rates are determined for various initial amounts of the acid at a constant enzyme concentration. A graph of 1/v versus the inverse of the keto acids concentration is shown below. Determine the Michaelis-Menten constant for this system. [HINT: For Michaelis-Menten kinetics, v= [M ] v max , where the Michaelis-Menten constant is KM.] K M + [M ] Rearrangement of the equation shows that 1 v = 1 v max KM v max + 1 [M ] . The plot should be a straight line with an intercept of 1 v max and a slope of KM . Hence, the Michaelis-Menten constant can be found from the v max following formula: KM = ( slope) /(intercept ) . To calculate the constant requires estimates of the slope and intercept of the plot. The intercept appears to be 3 0.2 min -1 micromole . Estimation of the slope is a little harder, but it seems to be about accuracy. This gives a slope of slope (1.1 10 ) mole 2 3 dm min (3.0) min 6 10 mole = (1.1 7.8 5.6 micromole mole to within about 10% 3 42 min dm mole 2 0.1) 10 6 dm 3 min . Then, from the formula 6 KM = = 0.36 mol . dm 3 But, of course there is a range since these are estimates. Conservatively, lets call it 15%. So, the range of correct answers is: 0.30 mol dm -3 < KM < 0.42 mol dm -3 Score for Page NAME: CHEM 444, Final Exam, Spring, 2011, page 6 6. (10 points) An experiment to determine the sedimentation coefficient of lysozyme at 20C was carried out by monitoring the movement of the boundary layer as a function of time while the sample was centrigfuged at 55,000 rpm. The data on the boundary distance from the pivot are given in the table. Determine the sedimentation coefficient of lysozyme. [Show all work. In particular, show an appropriate with plot, labels. Express your answer in the proper units.] Time (minutes) 0 30 60 90 120 150 Boundary distance from pivot (cm) 6.000 6.065 6.142 6.211 6.278 6.350 The boundary should move from the initial point by the following equation: 0.06 () = (0)(2 ) y = 0.0004x + 1E-05 0.05 ln(x/x(0)) 0.04 A plot of the logarithm of the ratio of the distance should 2 be a straight line with a slope equal to s . The plot is shown in the adjacent graph. The slope of this plot is -1 0.000379 min . 0.03 0.02 Next convert the rotation frequency to radians per second: 0.01 1 (2) = 5759.6 1 60 = 5.50 104 1 0 0 50 100 Time (min) 150 200 1 60 = 1.904 1013 2 Then, one finds the sedimentation coefficient to be = (0.000379 1 ) (5759.6 1 ) However, the proper unit of the sedimentation coefficient is the svedberg (= 110 s). So, the final answer is = 1.904 13 Score for Page NAME: CHEM 444, Final Exam, Spring, 2011, page 7 7. (15 points) In the following, carry out the mathematics requested as completely as possible. (a) 2 () = (2 /0 )(/20 ) Find the constant, A, that normalizes the radial part of the 2s wave function of the hydrogen atom: The normalization occurs when 2 = 1. Substitution of the function into this equation gives the following 0 equation: 2 (2 /0 )2 exp 2 = 1 0 0 One may simplify this equation by defining = /0 , which gives 3 2 0 (4 4 + 2 ) exp( ) 2 = 1 0 3 2 0 (4 2 4 3 + 4 ) exp( ) = 1 Multiplying through gives the following equation 0 Each of the three integrals in this formula can be found in Table 2.3. The result is 3 2 0 (4(2!) 4(3!) + 4!) = 1 Reducing this gives the equation 3 3 2 0 4(2!) = 2 0 (8) = 1 Rearranging this equation gives an expression for the normalization constant 1 = 3/ 2 220 (b) Determine the simplest form of the commutator, , 2 2 This is most easily done by carrying out the action on a general function, f: , () = = = + = = = Then, by comparison, the equivalent operator to the commutator must be , = Score for Page NAME: CHEM 444, Final Exam, Spring, 2011, page 8 8. (10 points) Match the statements/equations in part A with the names in part B by inserting the appropriate next to the statement. Part A Part B _b.__ Original explanation of the spectrum of hydrogen a. Borns hypothesis _f.__ Many-electron wave functions must be antisymmetric under the exchange of any two electrons. b. Bohr atom _e.__ _g.__ _d.__ = = c. Davisson-Germer experiment d. DeBroglies relation e. Heisenbergs principle f. Paulis principle g. Plancks relation Score for Page NAME: CHEM 444, Final Exam, Spring, 2011, page 9 9. (15 points) W hat is the probability that a quantum mechanical particle in a one-dimensional box will be found in the left quarter of the box through repeated measurements when it is in the lowest-energy state? [Show all work.] The probability of finding a particle within a region is the integral of the square of the wave function over that region. For the particle in one-dimensional box, this integral is 2 /4 2 /4 2 2 1 1 1 2 = = = 0, = 0 0 8 4 2 4 2 4 Score for Page NAME: CHEM 444, Final Exam, Spring, 2011, page 10 10. (10 points) (a) What is the ground-state configuration for a sodium atom? 2 2 6 1 (1s) (2s) (2p) (3s) (b) What term(s) arise(s) from this configuration? [HINT: Include the total angular momentum.] 2 The only term that arises is S1/2 (c) What are the next two excited configurations of the sodium atom? 2 2 6 1 (1s) (2s) (2p) (3p) 2 and 2 6 1 (1s) (2s) (2p) (4s) (d) What terms arise from these two configurations (including total angular momentum)? 2 P1/2 2 P3/2 2 and S1/2 (e) The spectrum of sodium has two rather strong transitions with wave lengths of 764.494 nm and 769.901 nm. From this information, calculate the spin-orbit coupling constant for the term that is split. 2 2 The term that is split is the P. These transitions are from that those terms down to the S1/2 term. According to the equation 2 2 in the handbook, the spin-orbit energy of the P1/2 is - , and the spin-orbit energy of the P3/2 term is /2. So, the difference in energy of the two terms arises from and energy splitting of 3/2. The energy difference is 1 1 769.901 764.494 = = = 9.186 106 1 764.494 769.901 764.494(769.901) Energies are not usually reported in these units, so one has to convert to a more convenient unit. 107 = 91.86 1 = 9.186 106 1 But the spin-orbit coupling constant is 2/3 of this value, so 2 = 91.86 1 = 61.24 1 3 Score for Page NAME: CHEM 444, Final Exam, Spring, 2011, page 11 11. (10 points) For the following molecules, write the ground configuration, its term symbol, and the bond order predicted by the aufbau principle. Molecule C2 F2 Ne2 O2 Ground Configuration 2 2 4 1 12 2 22 1 2 2 2 4 1 12 2 22 3 1 14 2 2 2 4 1 12 2 22 3 1 14 32 2 2 2 4 1 12 2 22 3 1 12 Term Symbol Bond Order g 2 g 1 g 0 g 2 1 1 1 3 Score for Page NAME: CHEM 444, Final Exam, Spring, 2011, page 12 12 16 12. (10 points) C O is the quintessential model of a heteronuclear diatomic molecule. From data in the handbook, predict -2 the vibrational force constant (assuming the harmonic approximation) of this molecule (in joules m ) as accurately as you can. Show all work. The equation that relates the force constant to measured properties is = (12.00000)(15.99491) = = 1.138505 1023 (6.02211415 1023 )(12.00000 + 15.99491) 0 ( + ) One can calculate the reduced mass of the molecule from the exact masses of the isotopes in Table 12.2. = -1 From Table 12.1, the vibrational frequency is 2170.21 cm . 2 = Rearranging the equation above, one obtains an expression for the force constant = 2(2.99792458 1010 1 )(2170.21 1 ) = 4.08792 1014 1 provided that one uses the proper units. The value of the vibrational frequency is = 1.138505 1026 (4.08792 1014 1 )2 = 1.90257 103 2 = 1.90257 103 2 Then, substitution gives Score for Page NAME: CHEM 444, Final Exam, Spring, 2011, page 13 13. (10 points, extra credit) From measurements of the differential cross section for scattering of electrons off atomic hydrogen, it was found that the atom has an electronic charge density given by (r) = exp(-r), where and are constants. (a) Find the relation between and such that the total charge equals e, the charge on the electron. (Express in terms of .) (b) Find the normalized wave function that describes this state in terms of these two parameters. ( ) 2 = (a) If one sums over all space, then the electron must be somewhere, so one has the requirement 0 ( ) 2 = Substitution of the form into this equation gives the following result 0 2! = 3 This can be integrated to give the following relationship: = So, in terms of , the answer is 3 2 (b) In order for the integrand to represent the probability of finding an electron at some point, the value must be proportional to an integral of the square of the wave function (= 1). That is, the density divided by e must be the square of the wave function. Hence, the wave function is () = () 3 () 3 = = ( /2) 2 2 Score for Page
Find millions of documents on Course Hero - Study Guides, Lecture Notes, Reference Materials, Practice Exams and more. Course Hero has millions of course specific materials providing students with the best way to expand their education.

Below is a small sample set of documents:

Delaware - CHEM - 444
Quantum Mechanics: Discretization of Energy and Wave-Particle Duality15th March 20101IntroductionClassical physics (derived from the ideas of Newton, Hamilton, Lagrange and other early physicists) encountered several experimental observations that it
Delaware - CHEM - 444
Quantum Mechanics: Discretization of Energy and Wave-Particle Duality15th March 20101IntroductionClassical physics (derived from the ideas of Newton, Hamilton, Lagrange and other early physicists) encountered several experimental observations that it
Delaware - CHEM - 444
Reaction Kinetics: Elementary Ideas10th February 20101IntroductionChemical equilibrium deals with chemical systems at equilibrium : that is,concentrations (and thus amounts) of chemical species do not change withtime.Chemical reaction kinetics atte
Delaware - CHEM - 444
Reaction Kinetics: Elementary Ideas25th February 20101Rate LawsReturning to our hypothetical model reaction:i i + j j k k + l lIn practice, the rate of reaction is treated as follows, thus introducingthe concept of the rate constant, k :Nreactants
Delaware - CHEM - 444
Kinetic Theory of Gases: Elementary Ideas17th February 201011.1Kinetic Theory: A Discussion Based on a Simplied View of the Motion of GasesPressure:Consul Engel and Reid (Ch. 33.1) for a discussion of the derivation for thepressure of a rareed coll
Delaware - CHEM - 444
Reaction Kinetics: Elementary Ideas18th February 20101Rate LawsReturning to our hypothetical model reaction:i i + j j k k + l lIn practice, the rate of reaction is treated as follows, thus introducingthe concept of the rate constant, k :N[i]iiR
Delaware - CHEM - 444
On Rate Constants: Simple Collision Theory,Arrhenius Behavior, and Activated ComplexTheory17th February 20100.1IntroductionUp to now, we havent said much regarding the rate constant k. It shouldbe apparent from the discussions, however, that: k is
Delaware - CHEM - 444
Kinetic Theory of Gases: Elementary Ideas9th February 201111.1Kinetic Theory: A Discussion Based on a Simplied View of the Motion of GasesPressure:Consul Engel and Reid (Ch. 33.1) for a discussion of the derivation for thepressure of a rareed colle
Delaware - CHEM - 444
Thermodynamics and kineticsThermodynamicsPhysical ChemistryLecture 4Introduction to chemical kineticsObserve relative stability of statesEnergy differencesStatic comparisons of statesKineticsObserve changes of state over timeSeveral different to
Delaware - CHEM - 444
Chemical kineticsPhysical ChemistryLecture 5Theoretical chemical kineticsTemperature dependence ofrate constantsk (T ) A exp( Ea / RT )Empirical theory ofArrhenius gives a usefulway to parameterizerate constantsA pre-exponentialfactorEa acti
Delaware - CHEM - 444
Elementary reactionsReactions of interest are often complexSome reactions do occur in a single step- elementary reactionsPhysical ChemistryLecture 6Reaction mechanisms andreaction-velocity predictionsMathematics of simplereaction sequencesSimple
Delaware - CHEM - 444
Physical ChemistryLecture 8Reactions in solution andrelaxation methods in fast kineticsThe cage effectIn solution, solventis a major factor inkineticsLimited proximity ofreactantsMolecules mustdiffuse into reactionzoneDiffusion controlLimiti
Delaware - CHEM - 444
The energy problemEarly experimentsPhysical ChemistryLecture 9Introduction to QuantumMechanicsObserved only certainemission frequenciesSpectra of atoms H and other atomsColors of mineralsolutionsScientists involvedhave very familiarnamesOth
Delaware - CHEM - 444
WavesPhysical ChemistryLecture 11Waves, Matrices, Operators, andEigenvalue Equations0n(0) -Wave moving through spacewavelength in vacuumrefractive index of the medium,which varies with wavelength (dispersion)Waves in complex notationWave equat
Delaware - CHEM - 444
Postulates of quantummechanicsAny state of a dynamical system of N particles isdescribed as fully as is possible by a function, ,such that the quantity *d3r is proportional to theprobability of finding r between r and r + d3r.For every observable pr
Delaware - CHEM - 444
Angular momentumVector property thatdescribes circularmotion of a particle or asystem of particlesRigid rotor model: Aparticle of mass m fixedto a massless rodExamples Swinging a bucket ofwater Movement of theEarth around the SunPhysical Chem
Delaware - CHEM - 444
Atomic configurationsMeans of describing the energy situation of a multi-electronsystemIndependent-electron energy is a sum of hydrogenic energies ofthe electronsPhysical ChemistryLecture 20Russell-Saunders Terms, Hunds Rules,Spin-orbit Coupling,
Delaware - CHEM - 444
Geometry of dihydrogenDihydrogenPhysical ChemistryFocus on translation andCoulombic interactionsLecture 22Diatomic MoleculesHTnme = mp/1836Good approximationCenter of massdetermined by thepositions of the nucleiCenter-of-mass problemis agai
Delaware - CHEM - 444
Delaware - CHEM - 444
Diatomic Molecules12th May 20091Hydrogen Molecule: Born-Oppenheimer ApproximationIn this discussion, we consider the formulation of the Schrodinger equation for diatomic molecules; this can be extended to larger molecules. First we will consider the s
Delaware - CHEM - 444
Quantum Mechanics: The Hydrogen Atom13th April 2011I. The Hydrogen AtomIn this next section, we will tie together the elements of the last severalsections to arrive at a complete description of the hydrogen atom. This will culminate in the denition of
Delaware - CHEM - 444
Helium Atom, Many-Electron Atoms, VariationalPrinciple, Approximate Methods, Spin21st April 2011I. The Helium Atom and Variational Principle: ApproximationMethods for Complex Atomic SystemsThe hydrogen atom wavefunctions and energies, we have seen, a
Delaware - CHEM - 444
Waves and the Schroedinger Equation5 april 20101The Wave EquationWe have seen from previous discussions that the wave-particle duality of matter requires we describe entities through some wave-form based represenation. The most natural consideration a
Delaware - CHEM - 444
Waves and the Schroedinger Equation5 april 20101The Wave EquationWe have seen from previous discussions that the wave-particle duality of matter requires we describe entities through some wave-form based represenation. The most natural consideration a
Delaware - CHEM - 444
CHEMISTRY 444.11QUIZ 3Spring, 2008 (08S)March 13, 2008NAME:Score _/151. (10 points)Consider the following reaction mechanism:k2A + A A *+Ak2A *+A A + A'k2A+ M A * + M'k2A * + M A+ Mk1A *B + Ca. Write an expression for the rate of react
Delaware - CHEM - 444
1Problem 1Do the one-dimensional kinetic energy and momentum operators commute?If not, what operator does their commutator represent?h2 d2KE =2m dx21.1dP = ihdxSolutionThis question requires calculating the commutator of the operators given.K
Delaware - CHEM - 444
1Problem 1The d orbitals have the nomenclature d z 2 , dxy , dxz ,dyz , and dx2 y2 . Showhow the d orbital given below can be written in the form y z F (r ).3dyz1.12=81 1ao3/2r 2 r/3aoesin( ) cos( ) sin()a2oSolutionz = r cos ( )x = r si
Delaware - CHEM - 444
1Problem 1In previous discussion, we have considered approximate methods for obtaining energies, wavefunctions, or both for quantum systems more complicatedthan the Hydrogen atom. In this exercise, consider the quantum harmonicoscillator and use the v
Delaware - CHEM - 444
1Problem 1For the atomic term 3 P , what are the energy dierences between the levelsarising due to spin-orbit coupling.1.1SolutionFor the atomic term 3 P , show the energy dierences between the levelsarising due to spin-orbit coupling.Answer For t
Delaware - CHEM - 444
CHEMISTRY 444.10/80QUIZ 1NAME:Spring, 2011February 18, 2011EMIL JANNINGSScore _/20[Numbers without decimal points are considered infinitely precise. Show reasonable significant figuresand proper units. Answers should be in reasonable units for the
Delaware - CHEM - 444
1Problem 1The rotational constant, Be , for IBr determined from microwave spectroscopyis 0.2241619 cm1 . Approximate the bond length of this molecule.1.1SolutionFrom the Handbook:Be =h28 2 ReRearranging gives the required form for solving for t
Delaware - CHEM - 444
Quiz Solutions: S10 (Section 011, CHEM444)27th February 20101Quiz 11.1Problem 1What is the ratio of the following values for a particle of Argon and Kryptonat 298K?AraveKraveArave=KraveArmostprobableArmostprobableKrmost83.798= 1.
Delaware - CHEM - 444
CHEMISTRY 444.11QUIZ 1Spring, 2011 (11S)Feb. 17, 2011NAME:Score _/20Problem 1 (8 points)Starting from the continuous probability distribution for one-dimensional diffusion, show how one woulddetermine the average squared displacement in a model de
Delaware - CHEM - 444
Quiz Solutions: S10 (Section 011, CHEM444)27th February 201011.1Quiz 1Problem 1What is the ratio of the following values for a particle of Argon and Krypton at 298K? Ar ave Kr aveAr ave = Kr avemKr = mAr83.798 = 1.45 39.948Ar most Kr mostproba
Delaware - CHEM - 444
Transport Properties: Momentum Transport,Viscosity13th February 20111IntroductionMuch as mass(material) is transported within uids (gases and liquids),linear momentum is also associated with transport, in this case, due togradients in velocity.See
Delaware - CHEM - 419
CORRECTIONS TO PHYSICAL CHEMISTRY FOR THE LIFE SCIENCES BYENGEL, DROBNY, AND REIDPage 337: The third sentence from the top of the page should read For E&lt; V(x) (insidethe box), the solutions have.Page 622: In Example Problem 24.1, the equation in the s
Delaware - CHEM - 419
CorrectionsEssential Data and Equations for a Course in PhysicalChemistryCecil Dybowski and Andrew V. TeplyakovPage 3-2, Table 3.41 joule = 9.47810-4 BTUPage 3-2, Table 3.61 Pa = 7.5006210-3 torr1 torr = 1.3157910-3 atm1 psi = 6.804610-2 atmPage
Delaware - CHEM - 419
NAME:KEY LARGOCHEMISTRY 419, SPRING, 2010 (2103)Examination 1, March 11,2010Answer each question in the space provided; use back of page if extra space is needed. Answer questions so the grader can READILYunderstand your work; only work on the exam
Delaware - CHEM - 419
NAME:MONKEYCHEMISTRY 419, SPRING, 2010 (2103)Midterm Examination 2, April 22, 2010Answer each question in the space provided; use back of page if extra space is needed. Answer questions so the grader can READILYunderstand your work; only work on the
Delaware - CHEM - 419
NAME:KEY, FRANCIS SCOTTCHEMISTRY 419, SPRING, 2010 (2103)Final Examination, May 22, 2010Answer each question in the space provided; use back of page if extra space is needed. Answer questions so the grader can READILYunderstand your work; only work o
Delaware - CHEM - 419
5/23/2010Student ID Midterm 1 Midterm 2 Quizzes Final Total5695153.55135.060.553700066944364040.538.238700101354927877.583.584700106045765850.563.764700127845554455.581.462700152593806975.574.775700170036535047.85
Delaware - CHEM - 419
Problem 24.2 part a 23k 1.3806505 10nm 101 J K23N 6.02211415 105M 0.131293 kgD 0.5 102 1m s3T 273 K1 3 8k T m a2mVaver 209.82sD 7.149 10Vaverk T2Problem 24.2 part bmN 2 1 N N 8k T m N2 P N0.0140067 kgN2 Vav
Delaware - CHEM - 419
Macroscopic characterizationwith distribution functionsPhysical ChemistryLecture 1Distributions and TransportProcessesParticles in a BoxExample distributionfunction for particles in abox, showing two regionsLeft side has more particlesthan the
Delaware - CHEM - 419
Macroscopic versus microscopicFicks laws describe timeevolution macroscopicallyPhysical ChemistryLecture 2Random walks; microscopictheory of diffusionDiffusion can be understoodin terms of a microscopicprocess the random walkProbability of event
Delaware - CHEM - 419
Origins of viscosityFluids try to achieve uniformflow across any region (i.e. aconstant speed independent ofposition)Fluids resist a gradient ofspeedsPhysical ChemistryLecture 3Viscosity and sedimentationDescribed by a drag force thatslows fast
Delaware - CHEM - 419
Electrophoresis in practiceGel electrophoresisPhysical ChemistryUses an acrylamide or agarose gelApply electric field for a given timeAfter electrophoresis, the gel isvisualized with a stainLecture 4Electrophoresis and lightscatteringFrom J. Vin
Delaware - CHEM - 419
RatesDescription of time dependence requires astatement of the time derivatives of theconcentrations of reactants and productsPhysical ChemistryLecture 5Introduction to chemical kineticsH2 ( gas) 1O ( gas) 22H2 O ( liquid )RatesRate of change
Delaware - CHEM - 419
Example Arrhenius plotPhysical ChemistryLecture 6Mechanisms of chemical reactionsUseful linear formSlope of plot givesthe activationenergy directlyMany rate constantsseem to obey thisrelationshipChemical kineticsUnderstand the nature of reacti
Delaware - CHEM - 419
Finding reaction velocityPhysical ChemistryLecture 7Multi-step reaction mechanismsOne knows the form of the reaction rate for everyelementary reactionExpress disappearance of reactant or appearance ofproduct in terms of the rates of these elementar
Delaware - CHEM - 419
Rate constants for bimolecularreactions in solutionReactionk (298 K)/ (dm3 mol-1 s-1)-H + HS H2S7.5 1010H+ + CH3OH CH3OH2+1 108OH- + HCO3- CO32- + H2O6 109Physical ChemistryLecture 8Reactions in solution andrelaxation methods in fast kinetic
Delaware - CHEM - 419
Pre-equilibrium approximationProduct formed only bysecond stepPhysical ChemistryElementary ratedetermined byintermediatesconcentrationABIIAssumption of rapidequilibriumLecture 9Kinetics of enzymatic reactionsSubstitution gives anexpression
Delaware - CHEM - 419
Absorption of energyEnergy is conserved in thetransfer of energy from theelectromagnetic field to amoleculePhysical ChemistryLecture 10Photochemistry and photophysicsin biological systemsAbsorption and emission onlyindicate energy differencesbe
Delaware - CHEM - 419
Photoelectric effectEmission of particles (electrons)by a metal due to interactionwith lightEinsteins explanation (for whichhe got the Nobel Prize) involvedassuming that the energy of aphoton was proportional to itsfrequencyPhysical ChemistryLec
Delaware - CHEM - 419
Conserved quantitiesQuantities that do not change in time are said to beconserveddp xExamples 0 p x is a conserved quantityPhysical ChemistrydtdEdtdp zdtLecture 12Mathematics of QuantumMechanics 0 E is a conserved quantity0p z is not cons
Delaware - CHEM - 419
Free particle in one dimensionFor a value of E there aretwo solutionsPhysical ChemistryLecture 13Solving Schroedingers Equationfor Simple SystemsGeneral solution for theenergy problem is a linearcombination of particularsolutionsNo limits on va
Delaware - CHEM - 419
Particle in three-dimensionalspaceThe world has threespatial dimensionsGeneralize simpleproblem to reflect thethree- dimensionalaspects of problemExample: a free particlein 3-D spaceAppropriate model for agas molecule in anunconfined spaceThe
Delaware - CHEM - 419
Particle in three-dimensionalspaceThe world has threespatial dimensionsGeneralize simpleproblem to reflect thethree- dimensionalaspects of problemExample: a free particlein 3-D spaceAppropriate model for agas molecule in anunconfined spaceThe
Delaware - CHEM - 419
Quantum angular-momentumoperatorsVector definitionsPhysical ChemistryLecture 15Angular momentum and the rigidrotorL Lx i L y j Lz kL2 L L L2 L2y L2xzExpression by correspondenceLxL2 i y z y z L2 L2 L2xyz i z x z xLyLz i x y x
Delaware - CHEM - 419
Particle in a finite 1-D boxFor E &gt; V0Wave functions are oscillatoryfunctions of xSums of exponential functions withimaginary argumentsAmplitudes are related by boundaryconditionsPhysical ChemistryFor E , it approaches thebehavior of the free pa
Delaware - CHEM - 419
Simplification of the hydrogenatom problemBy substitution, the hydrogen-atomHamiltonian becomesPhysical ChemistryHLecture 17The Hydrogen Atom, a CentralForce Problem12PCM2M H CM12p2 H relDecompose into two problemsH CM CM ECM CMH rel rel
Delaware - CHEM - 419
The helium atomConsists of a nucleus andtwo electronsHamiltonian has four kindsof terms Nuclear kinetic energy Electronic kineticenergy Nuclear-electronCoulombic potentialenergy Electron-electronCoulombic potentialenergyPhysical ChemistryLe