1 / 47

CHEM120 Midterm #2 Review November 10, 2010

CHEM120 Midterm #2 Review November 10, 2010. Outreach Trip. 2. Introduction. Marie Leung, SOS CHEM120 Coordinator/Tutor A little about me... Also a CHEM120L TA =) 4A Biomedical Sciences Glee Addict!. 3. 2. Outline of Session. Chapter 7: Thermochemistry introduction to energy systems

Download Presentation

CHEM120 Midterm #2 Review November 10, 2010

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. CHEM120 Midterm #2 Review November 10, 2010

  2. Outreach Trip 2

  3. Introduction • Marie Leung, SOS CHEM120 Coordinator/Tutor • A little about me... • Also a CHEM120L TA =) • 4A Biomedical Sciences • Glee Addict! 3 2

  4. Outline of Session • Chapter 7: Thermochemistry • introduction to energy systems • heats of reaction • pressure-volume work • first law of thermodynamics • enthalpy, ∆H & Hess’s Law 4 4

  5. Outline of Session • Chapter 8: Electrons in Atoms • electromagnetic radiation • introduction to quantum theory • quantum numbers and electron orbitals • electron configurations • Question and Answer Period 5 5

  6. Chapter 7: Thermochemistry 6

  7. Chapter 7: Thermochemistry • Introduction to Energy Systems • system vs surroundings • types of systems: • open system • closed system • isolated system • types of energy: • kinetic • thermal • potential 7

  8. Chapter 7: Thermochemistry • Heat • energy that is transferred between a system and its surroundings, as a result of a temperature difference • quantity of heat, q (in joules): • m= mass of substance (in grams) • c = specific heat capacity (in J/g•°C) • ∆t = change in temperature (°C) q = mc∆t 8

  9. Chapter 7: Thermochemistry • Heat • energy that is transferred between a system and its surroundings, as a result of a temperature difference • quantity of heat, q (in joules) • exothermic reaction: qrxn < 0 • endothermic reaction: qrxn > 0 q = mc∆t 9

  10. Chapter 7: Thermochemistry • Enthalpy, ∆H • measure of total energy of system • measured in kJ or kJ/mol (depending on situation) • q = quantity of heat (in joules) • n = moles ∆H = q/n 10

  11. Chapter 7: Thermochemistry • Heat ex. 1: Given 8.27 g of H2O (specific heat = 4.18 J/g•°C), how much heat is required to raise the temperature from 25°C to 99°C? 11

  12. Chapter 7: Thermochemistry • Heat & Law of Conservation of Energy • energy cannot be added to or taken away from the universe, but is simply transferred between a system and its surroundings qsystem + qsurroundings = 0 12

  13. Chapter 7: Thermochemistry • Heat & Law of Conservation of Energy ex. 2: A 1.22-kg piece of iron at 126.5°C is dropped into 981 g of water at 22.1°C. The temperature rises to 34.4°C. Determine the specific heat of iron, in J/g•°C. 13

  14. Chapter 7: Thermochemistry • Heat & Calorimetry ex. 3: The combustion of 1.010g sucrose (MC12H22O11 = 342.3g), in a bomb calorimeter causes the temperature to rise from 24.92°C to 28.33°C. The heat capacity of the calorimeter assembly is 4.90 kJ/°C. a. what is the heat of combustion of sucrose? b. how much energy is present in one teaspoon (i.e. 4.8g) of sucrose? 14

  15. Chapter 7: Thermochemistry • Pressure-Volume Work • work involved in the expansion or compression of gases Let’s think about a few scenarios... • constant volume (an isochoric process) w = -Pext x (0) = 0 = NO WORK! • constant pressure • isobaric expansion (∆V is positive) -Pext x (+V) = negative work • isobaric compression (∆V is negative) -Pext x (-V) = positive work w = -Pext x ∆V 15

  16. Chapter 7: Thermochemistry • Pressure-Volume Work ex. 4: How much work, in joules, is involved when 0.225 mol N2 (at a constant temperature of 23°C) is allowed to expand 1.50 L against a Pext of 0.750atm? 16

  17. Chapter 7: Thermochemistry • First Law of Thermodynamics • states the relationship between heat (q), work (w) and changes in internal energy (∆U) • in an isolated system, ∆U = 0, and thus, the energy of an isolated system is constant • sign conventions: • +q, +w: energy entering system (i.e. heat absorbed by system, or work done on system) • -q, -w: energy leaving system (i.e. heat released by system, or work done by system) ∆U = q+ w 17

  18. Chapter 7: Thermochemistry • First Law of Thermodynamics • ex. 5: In compressing a gas, 355 J of work is done on the system, while 185 J of heat is released from the system. Find ∆U. • sign conventions: 18

  19. Chapter 7: Thermochemistry • Enthalpy, ∆H • we know that: • under constant temperature and pressure: • therefore: ∆U = q+ w w = -P∆V qP = ∆H ∆U = ∆H- P∆V 19

  20. Chapter 7: Thermochemistry • Enthalpy, ∆H • ex. 6: For which of the following combustion reactions is ΔU = ΔH? A. CH4(g) + 2 O2(g) → CO2(g) + 2 H2O(l) B. C2H5OH(l) + 3 O2(g) → 2 CO2(g) + 3 H2O(l) C. C4H9OH(l) + 6 O2(g) → 4 CO2(g) + 5 H2O(l) D. none of the above 20

  21. Chapter 7: Thermochemistry • Hess’s Law & Heats of Formation • Guidelines: • 1. When reaction is multiplied or divided, multiply or divide ∆H by the same value. • 2. The sign for ∆H changes when reaction is reversed. • 3. When the reactions are summed together, the ∆H can be determined by summing together the ∆H of each individual reaction. 21

  22. Chapter 7: Thermochemistry • Hess’s Law & Heats of Formation • ex. 7: Find C2H4 (g) + H2 (g) C2H6 (g) C2H4 (g) + 3 O2 (g) 2 CO2 (g) + 2 H2O (l) ∆H = -1411 kJ C2H6 (g) + 7/2 O2 (g) 2 CO2 (g) + 3 H2O (l) ∆H = -1560 kJ H2 (g) + ½ O2 (g) H2O (l) ∆H = -285.8 kJ 22

  23. Chapter 8: Electrons in Atoms 23

  24. Chapter 8: Electrons in Atoms • Intro to Electromagnetic Radiation: • c = speed of light ≈ 3 x 108 m/s • ν = frequency (in s-1, or Hz) • λ = wavelength (in m) c = λν higher frequency shorter wavelength lower frequency longer wavelength 24

  25. Chapter 8: Electrons in Atoms Lawrence Berkeley National Laboratory http://www.lbl.gov/MicroWorlds/ALSTool/EMSpec/EMSpec2.html 25

  26. Chapter 8: Electrons in Atoms • Quantum Theory • Planck’s Equation • E = energy (in J) • h = Planck’s constant, 6.62607 x 10-34 J•s • note the trends: • shorter wavelength = higher frequency = higher energy • longer wavelength = lower frequency = lower energy E = hν = hc/λ 26

  27. HIGHEST ENERGY LOWEST ENERGY LOWEST FREQUENCY HIGHEST FREQUENCY LONGEST WAVELENGTH SHORTEST WAVELENGTH Chapter 8: Electrons in Atoms ...going back to the electromagnetic spectrum:

  28. Chapter 8: Electrons in Atoms • Electromagnetic Spectrum • Ex. 8: Which of the following has the highest energy? • A. red light • B. microwaves • C. ultraviolet radiation • D. radiowaves

  29. Chapter 8: Electrons in Atoms • Brief Overview of Quantum Mechanics • Heisenberg Uncertainty Principle: • we cannot know the exact position and momentum of an electron at the same time • that is, if we know one variable, we do not know the other

  30. Chapter 8: Electrons in Atoms • Quantum Numbers and Electron Orbitals • 1. principal quantum number, n • shell number • must be positive, nonzero integral value • n = 1, 2, 3, 4... • i.e. “the neighbourhood” 30

  31. Chapter 8: Electrons in Atoms • Quantum Numbers and Electron Orbitals • 2. orbital angular momentum quantum number, ι • may be zero or a positive integer • must not be larger than n-1 • ι = 0, 1, 2, 3... (n-1) • corresponds to subshells: • s: ι =0 • p: ι =1 • d: ι =2 • f: ι =3 • i.e. “the street” 31

  32. Chapter 8: Electrons in Atoms • Quantum Numbers and Electron Orbitals • 3. magnetic quantum number, mι • may be negative, zero or a positive integer • ranges from -ι to +ι • refers to number of orbitals • e.g. if ι =1 (i.e. p subshell), mι = -1, 0, 1 • thus, there are three p orbitals (and 2 electrons in each one - total 6 e-) • i.e. “the house” 32

  33. Chapter 8: Electrons in Atoms • Quantum Numbers and Electron Orbitals • 4. electron spin number, ms • either+1/2 or -1/2 • two electrons per orbital - spin in opposite directions 33

  34. Chapter 8: Electrons in Atoms • Quantum Numbers and Electron Orbitals • ex. 9: Which of the following sets of quantum numbers are allowed? • a. n = 3, ι = 2, mι = -1 • b. n = 1, ι = 2, mι = 0 • c. n = 4, ι = 4, mι = 3 • d. n = 1, ι = 0, mι = 0 • e. n = 2, ι = 1, mι = -1 34

  35. Chapter 8: Electrons in Atoms • Quantum Numbers and Electron Orbitals • wavefunction, Ψ • how electron behaves in orbital • electron density, Ψ2 • probability of finding electrons at one point at • distance r from nucleus • radial probability distribution, 4πr2Ψ2 • probability of finding electrons at all points distance • r from nucleus

  36. Chapter 8: Electrons in Atoms • Quantum Numbers and Electron Orbitals • the ORBITRON.... http://winter.group.shef.ac.uk/orbitron/

  37. Chapter 8: Electrons in Atoms Orbital Diagram 2s Dr. Richard Bader, McMaster University http://www.chemistry.mcmaster.ca/esam/Chapter_3/section_2.html Wavefunction (atomic orbital) Radial Probability Distribution Dr. Richard Oakley, University of Waterloo http://www.science.uwaterloo.ca/~oakley/chem120/notes/chapter_08.htm http://www.pci.tu-bs.de/aggericke/PC3e_osv/Kap_IV/Energiezustand.htm Take home message: s-orbitals Ψ, Ψ2 nonzero at r = 0!

  38. Chapter 8: Electrons in Atoms Orbital Diagram 2p Dr. Richard Bader, McMaster University http://www.chemistry.mcmaster.ca/esam/Chapter_3/section_2.html Wavefunction (atomic orbital) Radial Probability Distribution Dr. Richard Oakley, University of Waterloo http://www.science.uwaterloo.ca/~oakley/chem120/notes/chapter_08.htm http://www.pci.tu-bs.de/aggericke/PC3e_osv/Kap_IV/Energiezustand.htm

  39. Chapter 8: Electrons in Atoms Orbital Diagram 3d Dr. Richard Bader, McMaster University http://www.chemistry.mcmaster.ca/esam/Chapter_3/section_2.html Wavefunction (atomic orbital) Radial Probability Distribution Dr. Richard Oakley, University of Waterloo http://www.science.uwaterloo.ca/~oakley/chem120/notes/chapter_08.htm http://www.pci.tu-bs.de/aggericke/PC3e_osv/Kap_IV/Energiezustand.htm

  40. Chapter 8: Electrons in Atoms Orbital Diagram 4f Dr. Richard Bader, McMaster University http://www.chemistry.mcmaster.ca/esam/Chapter_3/section_2.html Wavefunction (atomic orbital) Dr. Richard Oakley, University of Waterloo http://www.science.uwaterloo.ca/~oakley/chem120/notes/chapter_08.htm

  41. Chapter 8: Electrons in Atoms • Electron Configurations • 1. Electrons fill orbitals in a way that minimizes the energy of the atom • the aufbau principle • i.e. lowest energy levels are filled first

  42. Chapter 8: Electrons in Atoms • Electron Configurations • 2. No two electrons in an atom may have the same four quantum numbers • the Pauli exclusion principle • n, ι and mι determine the electron orbital • electrons that share the first three quantum numbers belong to the same shell, subshell and orbital

  43. Chapter 8: Electrons in Atoms • Electron Configurations • 3. Within orbitals of identical energy, electrons will first fill them singly before pairing up • Hund’s Rule • stability is associated with half filled or fully filled orbitals

  44. Chapter 8: Electrons in Atoms • Electron Configurations • ex 10. Determine the elements denoted by the following electron configurations: • a. • b. 1s22s22p63s1

  45. Chapter 8: Electrons in Atoms • Electron Configurations • ex 11. Draw electron configurations for each of the following elements: • a. potassium • b. copper

  46. Question & Answer Period 44

  47. Good Luck! • Further Questions? • Marie (mariejasmineleung@gmail.com) • For more information on Waterloo Students Offering Support, visit http://www.waterloosos.com/ 45

More Related