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Chapter 16  pp Spontaneity, entropy and free energy Note:  For online HW, you  might  need to use the thermodynamic data sheet posted on my downloads website in the “helps” section  if  the values are not already in the problem.  You need to use ∆G values that have  at least one  decimal place and your textbook only goes to the “one’s” place.
Z5e 791 16.1 Methane and Oxygen React The products have lower potential energy than the reactants, resulting in energy flow (heat) to the surroundings.
16.1 Spontaneous ,[object Object],[object Object],[object Object],[object Object],[object Object]
Z5e 792 Figure 16.2 Rate of Reaction   Rate is a function of the pathway (kinetics) Spontaneity is a function of the potential energies (thermodynamics)
Thermodynamics ,[object Object],[object Object],[object Object],[object Object]
Entropy ,[object Object],[object Object],[object Object],[object Object]
[object Object],[object Object]
[object Object],[object Object],[object Object]
Figure 16.4 Three Possible Arrangements (states) of Four Molecules in a Two-Bulbed Flask (Each arrangement has several microstates as seen   in next slide)
[object Object],[object Object],[object Object]
Gases ,[object Object],[object Object],[object Object],[object Object]
Positional Entropy ,[object Object],[object Object],[object Object],[object Object],[object Object]
16.2 Entropy & 2nd Law of Thermodynamics ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Cell metabolism ,[object Object],[object Object]
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],pp
16.3 Temperature and Spontaneity ,[object Object],[object Object],[object Object],[object Object]
 S sys  S surr  S univ Spontaneous? - - - + + + + - ? Yes No, Reverse At  low  temp (  s surr   magnitude  >   S sys At  high  temp (  s sys   magnitude  >   S surr Z5e 803 Table 16.3   pp + - ?
16.4 Gibb's Free Energy ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Let’s Check ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Z5e 804 Table 16.4 ,[object Object],[object Object]
Predicting Spontaneity ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
 G =   H - T  S   pp + - At all Temp & exotherm + + At high temp & endoth.,  “ entropy driven” - - At low temperatures,  “ enthalpy driven” + - Not at any temperature, Reverse is spontaneous  H  S Spontaneous?
16.5 Entropy Changes in Chem. Rxns   pp ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Third Law of Thermo ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Z5e 810 Figure 16.6  H 2 O Molecule ,[object Object],[object Object]
16.6 Free Energy in Reactions ,[object Object],[object Object],[object Object],[object Object],[object Object]
Calculations Involving Energy If 2 mol reactants    4 mol product + 500 kJ, is the rxn likely spontaneous? Yes  What is the sign of ∆S rxn  when molten wax hardens? (-) How would your calculations change if the coefficients were not 1? ∆ H f  and S values in   Gº =   Hº - T  Sº multiplied by the coefficients.
Free Energy in Reactions   pp ,[object Object],[object Object],[object Object],[object Object],[object Object]
Free Energy in Reactions   pp ,[object Object],[object Object],[object Object],[object Object]
Three methods to determine G o   pp ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Three methods to determine G o   pp ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Three methods to determine G o   pp ,[object Object],[object Object],[object Object],[object Object],[object Object]
Z5e 16.7:  So Far . . .   pp ,[object Object],[object Object],[object Object],[object Object],[object Object]
16.7 Free energy and  Pressure   pp ,[object Object],[object Object]
16.7 Free energy and  Pressure   pp ,[object Object],[object Object],[object Object],[object Object],[object Object]
Free energy and  Pressure   pp ,[object Object],[object Object],[object Object],[object Object]
Free energy and  Pressure   pp ,[object Object],[object Object],[object Object],[object Object]
Free energy and  Pressure   pp ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
16.8 Free Energy &  Equilibrium   pp ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
5 Methods to Determine Gº   pp ,[object Object],[object Object],[object Object],[object Object],[object Object]
Figure 16.7  Balls Rolling Down into Two Types of Hills   ,[object Object],[object Object]
Z5e 820 16.8 The Dependence of Free Energy on Partial Pressure A (g)   B (g)   ,[object Object],[object Object],[object Object]
Figure 16.9 Free Energy and Equilibrium   a.   Gº  to reach =m, beginning with 1.0 mol  A (g )  & P A  = 2.0 atm b.   Gº  to reach =m, beginning with 1.0 mol  B (g)  & P B  = 2.0 atm c. G profile for A (g)     B (g)  with 1.0 mole of each at P total  =  2.0  atm.  Each point  on the curve corresponds to the  total  free energy of the system for a  given  combination  of A and B.
  Gº  K  ∆Gº = - RT ln(K) ,[object Object],[object Object],[object Object],= 1 > 1 < 1 pp
Free energy and equilibrium   pp ,[object Object],[object Object],[object Object],[object Object],[object Object]
Free energy and equilibrium   pp ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Free energy and equilibrium   pp ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Free energy and equilibrium   pp ,[object Object],[object Object],[object Object],[object Object],[object Object]
Free energy and equilibrium   pp ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Free energy and equilibrium   pp ,[object Object],[object Object],[object Object],[object Object],[object Object]
Temperature dependence  of K   pp ,[object Object],[object Object],[object Object],[object Object],[object Object]
16.9 Free energy And Work ,[object Object],[object Object],[object Object]
Figure 16.10 A Battery A  battery  can  do work  by sending current to a starter motor.  It can be  recharged  by  forcing  current through it in the  opposite  direction.
Figure 16.10 A Battery If the current flow in  both  processes is infinitesimally small, w1 = w2 and the process is  reversible
Figure 16.10 A Battery But, in  real  world, current flow is  finite , so w2 > w1 and process is  irreversible ; that is, the universe is  different  after the process occurs.
Figure 16.10 A Battery All real processes are irreversible.
Reversible v. Irreversible Processes   pp ,[object Object],[object Object],[object Object]

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Thermodynamics Chapter on Spontaneity, Entropy and Free Energy

  • 1. Chapter 16 pp Spontaneity, entropy and free energy Note: For online HW, you might need to use the thermodynamic data sheet posted on my downloads website in the “helps” section if the values are not already in the problem. You need to use ∆G values that have at least one decimal place and your textbook only goes to the “one’s” place.
  • 2. Z5e 791 16.1 Methane and Oxygen React The products have lower potential energy than the reactants, resulting in energy flow (heat) to the surroundings.
  • 3.
  • 4. Z5e 792 Figure 16.2 Rate of Reaction Rate is a function of the pathway (kinetics) Spontaneity is a function of the potential energies (thermodynamics)
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  • 9. Figure 16.4 Three Possible Arrangements (states) of Four Molecules in a Two-Bulbed Flask (Each arrangement has several microstates as seen in next slide)
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  • 17.  S sys  S surr  S univ Spontaneous? - - - + + + + - ? Yes No, Reverse At low temp (  s surr magnitude >  S sys At high temp (  s sys magnitude >  S surr Z5e 803 Table 16.3 pp + - ?
  • 18.
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  • 22.  G =  H - T  S pp + - At all Temp & exotherm + + At high temp & endoth., “ entropy driven” - - At low temperatures, “ enthalpy driven” + - Not at any temperature, Reverse is spontaneous  H  S Spontaneous?
  • 23.
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  • 27. Calculations Involving Energy If 2 mol reactants  4 mol product + 500 kJ, is the rxn likely spontaneous? Yes What is the sign of ∆S rxn when molten wax hardens? (-) How would your calculations change if the coefficients were not 1? ∆ H f and S values in  Gº =  Hº - T  Sº multiplied by the coefficients.
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  • 43. Figure 16.9 Free Energy and Equilibrium a.  Gº to reach =m, beginning with 1.0 mol A (g ) & P A = 2.0 atm b.  Gº to reach =m, beginning with 1.0 mol B (g) & P B = 2.0 atm c. G profile for A (g) B (g) with 1.0 mole of each at P total = 2.0 atm. Each point on the curve corresponds to the total free energy of the system for a given combination of A and B.
  • 44.
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  • 53. Figure 16.10 A Battery A battery can do work by sending current to a starter motor. It can be recharged by forcing current through it in the opposite direction.
  • 54. Figure 16.10 A Battery If the current flow in both processes is infinitesimally small, w1 = w2 and the process is reversible
  • 55. Figure 16.10 A Battery But, in real world, current flow is finite , so w2 > w1 and process is irreversible ; that is, the universe is different after the process occurs.
  • 56. Figure 16.10 A Battery All real processes are irreversible.
  • 57.