Thermodynamic favorability and temperature

0:00- [Instructor] The thermodynamic favorability of a chemical reaction can be affected by the temperature. Let's say we have a generic reaction where the reactants turn into the products. As a quick review, when the standard change in free energy, delta G naught, is less than zero, the forward reaction is thermodynamically favorable.

0:19Therefore, the net reaction goes to the right to make more of the products. And when delta G naught is greater than zero, the forward reaction is thermodynamically unfavorable. That means that the reverse reaction is favorable and the net reaction would go to the left to make more of the reactants.

0:37One way to calculate delta G naught is to use the following equation. Delta G naught is equal to delta H naught minus the absolute temperature times delta S naught. And since delta H naught is talking about the standard change enthalpy, for this equation delta H naught will be called the enthalpy term.

0:56And because delta S naught is talking about the standard change in entropy, the absolute temperature times delta S naught will be referred to as the entropy term. So when we're trying to figure out if delta G naught is negative or if delta G naught is positive, we need to consider the sign for delta H naught, the sign for delta S naught, and sometimes we also need to consider what the temperature is.

1:22There are four possible combinations of signs for delta H naught and delta S naught as we can see in this table. For each of these four combinations, we're gonna think about the temperatures at which delta G naught is less than zero and we're gonna finish filling out this table.

1:37To start with, we're gonna think about the situation where delta H naught is negative and delta S naught is positive. So for this first possible combination, when delta H naught is negative, we say that's an exothermic reaction. And when delta S naught is positive, that's saying there's an increase in entropy as reactants turn into products.

2:00So let's think about the sign for delta G naught if we plug in some numbers for delta H naught, temperature, and delta S naught. And when I plug in some numbers, I'm not really concerned about a particular reaction. I'm not concerned about units. I'm not concerned about significant figures.

2:15I'm just interested in looking at the numbers and seeing how the math affects the sign for delta G naught. So for delta H naught, I'm saying that's -100. For T, I'm saying that's 100, and for delta S naught, I'm saying that's +0.1. So this would be equal to -100 - 10, which is equal to -110.

2:43So delta G naught is negative. Notice how a negative entropy term favors getting a negative value for delta G naught. And notice how a positive entropy term, since we're subtracting that in our equation is also favorable for getting a negative value for delta G naught.

3:03Also notice, no matter what we put in for the temperature since delta S naught is positive, the entropy term will always be positive. And since we're subtracting it in our equation, we would always get a negative value for delta G naught. So whenever delta H naught is negative and when delta S naught is positive, delta G naught will be negative no matter what the temperature.

3:29So if we go back to our chart for our first possible combination, when delta H naught is negative, that's favorable. And when delta S naught as positive, that's also favorable. Therefore delta G naught is less than 0 at all temperatures. So I'm gonna go ahead and write in here, 'at all temperatures' in our chart.

3:47As an example of this, let's consider the conversion of ozone gas into oxygen gas. Since energy is released, this is an exothermic reaction, and delta H naught is negative. And since we're going from 2 moles of gas on the reactant side to 3 moles of gas on the product side, that's an increase in entropy.

4:08So delta S naught is positive. Since delta H naught is negative and delta S naught is positive, delta G naught for this reaction is less than zero at all temperatures. That means the forward reaction is thermodynamically favorable, and ozone gas would turn into oxygen gas, and this reaction would occur at all temperatures.

4:31The second possible combination for the signs is when delta H naught is positive and when delta S naught is negative. When delta H naught is positive, that's an endothermic reaction. And when delta S naught is negative, there's a decrease in entropy going from reactants to products.

4:49Once again we're gonna plug in some numbers and solve for delta G naught. So for delta H naught, let's say that's +100, for the temperature term, let's say that's 100, and delta S naught, let's say that's -0.1. When we do the math, we get positive 100 - negative 10, which is equal to +110.

5:18So delta G naught is positive. Notice when the entropy term is positive, that's not favorable for getting a negative value for delta G naught. And when the entropy term is negative, since we're subtracting this negative, we would actually be adding the entropy term.

5:37And that would not favor a negative value for delta G naught. Also notice, no matter what you put in for the temperature here, you're always gonna get a negative value for the entropy term. And if the enthalpy term is positive, since we would mathematically be adding the entropy term, we would always get a positive value for delta G naught.

5:57So whenever delta H naught is positive and delta S naught is negative, delta G naught will be positive no matter what the temperature. So going back to our charge when delta H naught is positive, that was not favorable, and when delta S naught was negative, that was also not favorable.

6:16So it doesn't matter what the temperature is. Delta G naught will not be less than zero. Therefore, on our chart here we can write in, at no temperature will delta G naught be less than zero. As an example of this, let's look at the reverse of the reaction we saw for the first possible combination.

6:34Before we had ozone turning into oxygen gas, and now we have oxygen gas turning into ozone. Because heat is on the reactant side, we know this reaction is endothermic and delta H naught is positive. And since we're going from 3 moles of gas on the reactant side to 2 moles of gas on the product side, that's a decrease in entropy, and delta S naught is negative.

6:58Since delta H naught is positive and delta S naught is negative, delta G naught will never be less than zero. It doesn't matter what the temperature is. And so the forward reaction is always thermodynamically unfavorable. The third possible combination of signs has both delta H naught and delta S naught as being negative.

7:19Once again we're gonna plug some numbers into the equation and see what happens to the sign of delta G naught. So let's say delta H naught is -100. The temperature is 100 and delta S naught is -0.1. Doing the math, we get negative 100 minus negative 10. So that's -100 + 10, which is equal to -90.

7:40Let's think about why we got a negative value for delta G naught. The enthalpy term is negative, which favors a negative value for delta G naught. The entropy term is also negative, but since we're subtracting the entropy term, it actually gets added for the overall delta G naught calculation.

7:59So the entropy term is not favorable. However, in this case, the favorable entropy term outweighs the unfavorable entropy term. And that's the reason why we get a negative value for delta G naught at this temperature. Let's compare the calculation that we just did at a temperature of 100, which gave us a negative value for delta G naught, to a similar calculation, except this time we have a much higher temperature.

8:26This time it's 2000. But notice how the values for delta H naught and delta S naught are the same as before. The reason why we can use the same values at a different temperature is because delta H and delta S naught don't change much with temperature. However, delta G naught does change a lot with temperature.

8:45Because at this higher temperature, when we do the math, we see that now we get delta G naught is equal to +100. So at this higher temperature, even though the enthalpy term is favorable, now the unfavorable entropy term outweighs the favorable enthalpy term and gives us a positive value for delta G naught.

9:07Therefore, at a relatively lower temperature, delta G naught is negative. However, at a higher temperature, delta G naught is positive. So when delta H naught is negative, that's favorable, but when delta S naught is negative, that's not favorable. And we just saw from the calculations that delta G naught will be negative at low temperatures.

9:29So let's write that in here in our chart. So far we've been talking about delta G naught relative to a chemical process. However, delta G naught also applies to a physical process. In this case we're looking at liquid water turning into solid water. So this is the process of freezing.

9:48The process of freezing gives off energy. So this process is exothermic, and delta H naught will be negative. Going from a liquid to a solid is a decrease in entropy, therefore, delta S naught is negative. For this combination of signs, delta G naught is negative only at relatively low temperatures.

10:09Therefore, the forward process of freezing is thermodynamically favorable at low temperatures. And this matches with what we already know about water, water freezes at a relatively low temperature. Finally, let's look at our fourth combination of signs, and that's when both delta H naught and delta S naught are positive.

10:30So let's say delta H naught is equal to +100, delta S naught is equal able to +0.1, and first we'll look at the lower temperature of 100. Doing the math, we get positive 100 - 10, which gives us a positive value for delta G naught. And if we do the calculation at a higher temperature of 2000, notice that delta H naught is still +100 and delta S not is still +0.1.

10:55This time we get -100 for delta G naught. Notice how for this example at the higher temperature, the entropy term is unfavorable for giving a negative value for delta G naught. However, the entropy term is favorable. A positive value for delta S naught gives a positive value for the entropy term.

11:14And since we are subtracting it, the entropy term outweighs the enthalpy term, giving a negative value for delta G naught. However, for the first example at the lower temperature, since the temperature is lower, the entropy term is a smaller value, and is unable to overcome the unfavorable enthalpy term.

11:35And that's the reason why delta G naught ends up being positive at the lower temperature. So for this combination of signs, delta G naught is negative at higher temperatures. So for our fourth combination, when delta H naught is positive, that is unfavorable. However, when delta S naught is positive, that is favorable.

11:56And we just saw that delta G naught is less than zero at high temperatures. So I'll go ahead and write in on our table here, 'at high temperatures.' As an example of this, let's consider solid water turning into liquid water. So the forward process is the process of melting.

12:16It takes energy to disrupt the intermolecular forces of the solid, therefore, heat is on the reactant side and delta H naught is positive. Melting is an endothermic process. Going from a solid to a liquid is an increase in entropy. Therefore, delta S naught is positive.

12:35And when both signs are positive, our calculations showed us that delta G naught is less than zero at high temperatures. Therefore, the forward process of melting is thermodynamically favorable at relatively high temperatures. And this matches what we already know from experience.

12:53At relatively low temperatures ice does not melt. However, at relatively high temperatures ice does melt. Now that we have our chart filled out, let's summarize what we've learned about these four possible combinations. When delta H naught and delta S naught are both favorable, the forward process is thermodynamically favorable at all temperatures.

13:15When delta H naught and delta S naught are both unfavorable, the forward process is thermodynamically favorable at no temperatures, or you could say the forward process is thermodynamically unfavorable at all temperatures. When delta H naught is favorable and delta S naught is unfavorable, the forward process is only thermodynamically favorable at low temperatures.

13:42And finally, if delta H naught is unfavorable, but delta S naught is favorable, the forward process is thermodynamically favorable only at high temperatures.