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The ICE table is as follows: H 2 I 2 HI 601
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The ICE table is as follows: H 2 I 2 HI 602
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The ICE table is as follows: H 2 I 2 HI 0.00623 – y 0.00414 – y 0.0224 + 2y 603
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The ICE table is as follows: H 2 I 2 HI 0.00623 – y 0.00414 – y 0.0224 + 2y 604
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Now think about any possible simplification. 605
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Now think about any possible simplification. There is none! 606
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Math Aside: The quadratic equation 607
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Math Aside: The quadratic equation A quadratic equations looks like: 608
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Math Aside: The quadratic equation A quadratic equations looks like: 609
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Math Aside: The quadratic equation A quadratic equations looks like: The solutions (there are two of them) take the form 610
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Math Aside: The quadratic equation A quadratic equations looks like: The solutions (there are two of them) take the form 611
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Math Aside: The quadratic equation A quadratic equations looks like: The solutions (there are two of them) take the form Note that in an equilibrium problem, only one of the solutions will generate a physically acceptable solution to the problem. 612
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We now need to solve 613
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We now need to solve 614
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We now need to solve 615
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We now need to solve 616
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We now need to solve Now solve the quadratic equation using with a = 50.3, b = -0.653, and c = 8.99x10 -4. 617
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618
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y = 0.0114 M or y = 0.00157 M. 619
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y = 0.0114 M or y = 0.00157 M. The first answer is physically impossible. 620
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y = 0.0114 M or y = 0.00157 M. The first answer is physically impossible. Why? 621
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y = 0.0114 M or y = 0.00157 M. The first answer is physically impossible. Why? The concentration of I 2 = 0.00414 – y = -0.00726 M which is physically impossible. We cannot have a negative concentration. 622
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y = 0.0114 M or y = 0.00157 M. The first answer is physically impossible. Why? The concentration of I 2 = 0.00414 – y = -0.00726 M which is physically impossible. We cannot have a negative concentration. So the solution we seek is y = 0.00157 M. 623
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At equilibrium: 624
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At equilibrium: [H 2 ] = 0.00623 – 0.00157 = 0.00466 M 625
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At equilibrium: [H 2 ] = 0.00623 – 0.00157 = 0.00466 M [I 2 ] = 0.00414 – 0.00157 = 0.00257 M 626
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At equilibrium: [H 2 ] = 0.00623 – 0.00157 = 0.00466 M [I 2 ] = 0.00414 – 0.00157 = 0.00257 M [HI] = 0.0224 + 2x 0.00157 = 0.0255 M 627
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At equilibrium: [H 2 ] = 0.00623 – 0.00157 = 0.00466 M [I 2 ] = 0.00414 – 0.00157 = 0.00257 M [HI] = 0.0224 + 2x 0.00157 = 0.0255 M Check: 628
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At equilibrium: [H 2 ] = 0.00623 – 0.00157 = 0.00466 M [I 2 ] = 0.00414 – 0.00157 = 0.00257 M [HI] = 0.0224 + 2x 0.00157 = 0.0255 M Check: 629
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There is a simple way to tell which way the reaction will proceed to equilibrium. 630
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There is a simple way to tell which way the reaction will proceed to equilibrium. Consider H 2(g) + I 2(g) 2 HI (g) and suppose all three gases are present at the start of the reaction. 631
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There is a simple way to tell which way the reaction will proceed to equilibrium. Consider H 2(g) + I 2(g) 2 HI (g) and suppose all three gases are present at the start of the reaction. The reaction quotient is where the initial concentrations are employed. 632
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There is a simple way to tell which way the reaction will proceed to equilibrium. Consider H 2(g) + I 2(g) 2 HI (g) and suppose all three gases are present at the start of the reaction. The reaction quotient is where the initial concentrations are employed. If Q c > K c there must be too much HI in the mixture for equilibrium to exist. Consequently, the reaction will proceed from right to left, until Q c becomes equal to K c. 633
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There is a simple way to tell which way the reaction will proceed to equilibrium. Consider H 2(g) + I 2(g) 2 HI (g) and suppose all three gases are present at the start of the reaction. The reaction quotient is where the initial concentrations are employed. If Q c > K c there must be too much HI in the mixture for equilibrium to exist. Consequently, the reaction will proceed from right to left, until Q c becomes equal to K c. If Q c < K c, the reaction will proceed left to right. 634
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In many equilibrium problems, the equilibrium constant is very small. This allows a simplification of the mathematics, so that the general quadratic equation does not have to be solved. 635
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In many equilibrium problems, the equilibrium constant is very small. This allows a simplification of the mathematics, so that the general quadratic equation does not have to be solved. Example 3: 1.00 moles of N 2 is placed in a 1.00 liter vessel along with 1.10 moles of O 2 at 25 o C. Calculate the amount of NO formed at 25 o C. K c = 4.8 x 10 -31 at 25 o C for the reaction N 2(g) + O 2(g) 2 NO (g). 636
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The ICE table is as follows: N 2 O 2 NO 637
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The ICE table is as follows: N 2 O 2 NO 638
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The ICE table is as follows: N 2 O 2 NO 639
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The ICE table is as follows: N 2 O 2 NO 1.00 – y 1.10 – y 2y 640
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The ICE table is as follows: N 2 O 2 NO 1.00 – y 1.10 – y 2y 641
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Now 642
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Now At this point, always stop and look for any possible simplifications. 643
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Now At this point, always stop and look for any possible simplifications. Notice that we do not have a perfect square on the right-hand side. 644
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Now At this point, always stop and look for any possible simplifications. Notice that we do not have a perfect square on the right-hand side. In this case there is a mathematical simplification on the right-hand side of the equation – 645
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Now At this point, always stop and look for any possible simplifications. Notice that we do not have a perfect square on the right-hand side. In this case there is a mathematical simplification on the right-hand side of the equation – what is it? 646
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Now At this point, always stop and look for any possible simplifications. Notice that we do not have a perfect square on the right-hand side. In this case there is a mathematical simplification on the right-hand side of the equation – what is it? Notice that K c is very small, which means very little product will be formed. 647
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Since y is very small, we try the approximations: 1.00 – y 1.00 1.10 – y 1.10 648
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Since y is very small, we try the approximations: 1.00 – y 1.00 1.10 – y 1.10 We will check momentarily the quality of these approximations. The equilibrium constant expression simplifies to 649
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Since y is very small, we try the approximations: 1.00 – y 1.00 1.10 – y 1.10 We will check momentarily the quality of these approximations. The equilibrium constant expression simplifies to K c 650
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Since y is very small, we try the approximations: 1.00 – y 1.00 1.10 – y 1.10 We will check momentarily the quality of these approximations. The equilibrium constant expression simplifies to K c 651
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Since y is very small, we try the approximations: 1.00 – y 1.00 1.10 – y 1.10 We will check momentarily the quality of these approximations. The equilibrium constant expression simplifies to K c So y = 3.6 x 10 -16 M. 652
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Since y = 3.6 x 10 -16 M the approximations 1.00 – y 1.00 1.10 – y 1.10 are justified. At equilibrium: [NO] = 2 y = 7.2 x 10 -16 M 653
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When can approximations be made to simplify equilibrium constant expressions? 654
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When can approximations be made to simplify equilibrium constant expressions? The only places where approximations can be made are (where A and B are concentrations): 655
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When can approximations be made to simplify equilibrium constant expressions? The only places where approximations can be made are (where A and B are concentrations): (A – y) A where A >> y 656
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When can approximations be made to simplify equilibrium constant expressions? The only places where approximations can be made are (where A and B are concentrations): (A – y) A where A >> y and (B + y) B where B >> y 657
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When can approximations be made to simplify equilibrium constant expressions? The only places where approximations can be made are (where A and B are concentrations): (A – y) A where A >> y and (B + y) B where B >> y Never in places like y (A – y) or 658
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Le Châtelier’s Principle 659
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Le Châtelier’s Principle We will examine the effect of the following on the equilibrium constant. 660
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