1 / 11

Maximum Work

Maximum Work. Often reactions are not carried out in a way that does useful work. As a spontaneous precipitation reaction occurs, the free energy of the system decreases and entropy is produced, but no useful work is obtained.

wylie-avery
Download Presentation

Maximum Work

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. Maximum Work • Often reactions are not carried out in a way that does useful work. • As a spontaneous precipitation reaction occurs, the free energy of the system decreases and entropy is produced, but no useful work is obtained. • In principle, if a reaction is carried out to obtain the maximum useful work, no entropy is produced.

  2. Maximum Work • Often reactions are not carried out in a way that does useful work. • It can be shown that the maximum useful work,wmax , for a spontaneous reaction isDG. • The term free energy comes from this result.

  3. Free Energy Change During Reaction • As a system approaches equilibrium, the instantaneous change in free energy approaches zero. • Figure 19.9 illustrates the change in free energy during a spontaneous reaction. • As the reaction proceeds, the free energy eventually reaches its minimum value. • At that point,DG= 0, and the net reaction stops; it comes to equilibrium.

  4. Relating DGo to the Equilibrium Constant The free energy change when reactants are in non-standard states (other than 1 atm pressure or 1 M) is related to the standard free energy change, DGo, by the following equation. • Here Q is the thermodynamic form of the reaction quotient.

  5. Relating DGo to the Equilibrium Constant • The free energy change when reactants are in non-standard states (other than 1 atm pressure or 1 M) is related to the standard free energy change, DGo, by the following equation. • DGrepresents an instantaneous change in free energy at some point in the reaction approaching equilibrium.

  6. Relating DGo to the Equilibrium Constant • The free energy change when reactants are in non-standard states (other than 1 atm pressure or 1 M) is related to the standard free energy change, DGo, by the following equation. • At equilibrium,DG=0and the reaction quotient Q becomes the equilibrium constant K.

  7. Relating DGo to the Equilibrium Constant • The free energy change when reactants are in non-standard states (other than 1 atm pressure or 1 M) is related to the standard free energy change, DGo, by the following equation. • At equilibrium,DG=0and the reaction quotient Q becomes the equilibrium constant K.

  8. Relating DGo to the Equilibrium Constant • This result easily rearranges to give the basic equation relating the standard free-energy change to the equilibrium constant. • When K > 1 , the ln K is positive andDGois negative. • When K < 1 , the ln K is negative andDGo is positive.

  9. Spontaneity and Temperature Change • All of the four possible choices of signs for DHo and DSo give different temperature behaviors for DGo.

  10. You get the value ofDGToat any temperature T bysubstituting values ofDHoandDSoat 25 oC into the following equation. Calculation of DGo at Various Temperatures • In this method you assume that DHo and DSo are essentially constant with respect to temperature.

  11. DHfo: -1206.9 -635.1 -393.5 kJ So: 92.9 38.2 213.7 J/K A Problem To Consider • Find the DGo for the following reaction at 25oC and 1000oC. Relate this to reaction spontaneity.

More Related