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### Vapor Pressure of Solutions

Lecture Slides are screen-captured images of important points in the lecture. Students can download and print out these lecture slide images to do practice problems as well as take notes while watching the lecture.

• Intro 0:00
• Vapor Pressure of Solutions 2:07
• Vapor Pressure & Raoult's Law
• Example 1
• When Ionic Compounds Dissolve
• Example 2
• Non-Ideal Solutions
• Negative Deviation
• Positive Deviation
• Example 3

### Transcription: Vapor Pressure of Solutions

Hello, and welcome back to Educator.com; welcome back to AP Chemistry.0000

Today, we are going to be talking about the vapor pressure of solutions.0003

Now, we have talked about vapor pressure before, and that is basically: at any given temperature, there is always going to be some of the molecules on the surface of a liquid that have escaped into the gas phase.0008

So, in a closed container, there is always going to be some gas above the particular liquid--like, if I have water in a closed container, yes, you see the liquid water there; but on top of the liquid water, there is a little bit of water vapor, at every temperature--not just at 100 degrees Celsius.0018

100 degrees Celsius is the boiling temperature of water; that is when every single molecule of liquid water has enough energy to go and stay in the vapor state.0036

But, in every liquid, there is always some amount of gas above it.0045

Well, again, pressure is just a measure of the number of particles in a particular closed container; so we call that thing the vapor pressure of the solvent.0051

Well, today we are going to be talking about the vapor pressure of solutions; if you take a non-volatile solute (like if you take salt and dissolve it in some water), that actually ends up changing the vapor pressure of the solvent.0059

Now, you can call it different things, and in the process of discussing it, sometimes I'm going to say "vapor pressure of solute"; sometimes I'm going to say "vapor pressure of solution"; we'll know what we are talking about if we are talking about pure solvent or some solution.0071

But, in essence, when I put a solute (like salt) in water and dissolve it, now the water molecules are actually competing with other particles (namely, the sodium ion and the chloride ion) to make their way up to the surface, so they can actually escape into the gas phase.0086

Well, because these ions are actually running interference, not as many water molecules make it to the surface; therefore, not as many jump up into the vapor phase; therefore, the vapor pressure (which is a measure of how much is on top of the liquid at any given time) is going to be lower, in general.0104

Let's go ahead and get started; that is just a quick description of what it is that we are going to do.0122

OK, so let's write down: the vapor pressure of a...no, not "the vapor pressure of a"...what am I saying here?--I can't write that.0127

The presence (I'm getting ahead of myself) of a non-volatile solute (and non-volatile means, generally, it is not a liquid; it's a solid of some sort--a salt or sugar--some covalent compound that forms a crystal) lowers the vapor pressure of the solvent.0148

And again, if you need to do a quick review of vapor pressure, just go back some lessons, where we actually talk about what vapor pressure is.0184

We have actually also talked about it twice, if you remember--when we did gases, when we were collecting a gas above a liquid and using that technique of displacement to measure the volume of a gas, we talked about vapor pressure then.0191

So, we have actually discussed it a couple of times.0203

All right, vapor pressure of a solvent...now, this is our important equation: it's something called Raoult's Law, and it goes something like this.0207

You know what, I'm always worried when I use different variables; I actually like to write my variables out; I don't really care for letters, myself, personally--because there are so many letters in science that you collect, after a certain number of classes, that they tend to get confusing.0218

Well, you know what, let me just go ahead and leave it as I have.0236

The vapor pressure of the solution is equal to the mole fraction of the solvent (it's very, very important to identify, because now we have solvent and solute; we have to specify what we are talking about), times the initial vapor pressure of the solvent.0240

So, Raoult's Law says that, if I have a particular solution, and there is some solute that has been put into solvent to create the solution, the vapor pressure that I end up measuring under ideal conditions--it will be: I take the normal vapor pressure of the pure solvent, and I multiply it by the mole fraction of the solvent.0258

So now, the mole fraction is no longer 1; there is actually solvent and solute in the solution; therefore, the mole fraction is going to be less than 1.0283

Remember what mole fraction is: the moles of the A over the total moles.0295

So, in this case, it's going to be the moles of solvent over moles of solute plus moles of solvent.0299

It is going to be less than 1, so your pressure is actually going to be less than the normal pressure, which makes sense, because again, molecules--the solvent molecules--are interfering with the solvent molecules' ability to get to the surface so they can jump up into the vapor phase.0305

Let's do an example.0321

We'll do Example 1: OK, now, what is the expected vapor pressure (I'll just call it V/P) at 25 degrees Celsius, for a sucrose solution of 120.0 grams of sucrose, dissolved in (oops, it's not 572; I want...) 527.0 milliliters of water?0326

OK, now we're going to have some information that we need here: At 25 degrees Celsius, the density of water (that's a little Greek delta) equals 0.9971 grams per milliliter.0374

The vapor pressure, the normal vapor pressure, of H2O (the solvent) equals 23.76 torr.0393

That means that, at 25 degrees Celsius (just really briefly), if I have a glass of water that is covered, at 25 degrees Celsius, the amount of vapor--water vapor--above the liquid in the glass actually accounts for 23.76 torricelli.0407

Not a lot, but it is some pressure; it is some gas particles that are bouncing around, hitting the walls of the container, causing a pressure; that is what vapor pressure is.0425

It is the measure of how much vapor is actually above a liquid at a given temperature.0434

Sorry to keep repeating myself, but I find that repetition sort of enforces comfort with these things.0439

Now, sucrose (which is just normal table sugar--so we're just making a sugar solution) is 342.3 grams per mole; so these are the things that we are going to need.0447

OK, so Raoult's Law: this is the law that we are going to use; let me go ahead and circle this in red.0460

That is what we want to use; so we need to find--we have this one already; that is the 23.76 torr; we need to find the mole fraction of water, the solvent.0465

We go...so we are going to need to find, first of all, the moles of sucrose; well, the moles of sucrose--we said we had 120 grams, times 1 mole (nice stoichiometric conversion), over 342.3 grams; that gives us 0.3506 mol.0478

You know, let me write my numbers a little bit bigger; I think they might be a little tiny here: 0.3506 moles of sucrose.0500

OK, now we need the moles of H2O.0509

Well, H2O...we have 527 milliliters, so we need to convert that to grams first, so that is why we need the density.0513

We have 0.9971 grams per milliliter, times (grams goes down here; mol goes up there) 18 grams in 1 mole; so it's going to be 527, times .9971, divided by 18; and we get 29.193 moles.0521

29.193 mol: therefore, the mole fraction of H2O is equal to the number of moles of water, divided by the total moles (which is 29.193+0.3506).0543

When I do that, I get 0.9881; so it's going to be less than 1; it's a fraction--it's a part over the whole.0565

If we wanted the mole fraction of sucrose, well, we would say .3506 in the numerator; the denominator is the total moles; I hope that is OK.0574

OK, so now, when we plug this into the equation, the vapor pressure of the solution is going to be 0.9881 (which is the mole fraction of water), times the normal vapor pressure at that temperature (23.76), and we end up with 23.47 torricelli (or torr, or millimeters of mercury...if you want to convert that to atmospheres, psi, kilopascal, whatever you need; it's just a unit of pressure).0583

Notice, 23.47 is not a lot less than 23.76, but it is less.0615

That is what is important: when you add a solute to a solvent (in other words, when you create a solution--a non-volatile solute), your vapor pressure will lower.0621

What that means is that fewer molecules of liquid will hang around in the vapor state on top of the liquid, because fewer molecules will be able to get to the surface, because the molecules of solute are getting in their way, so they can't jump up as much.0633

OK, now, this was for a covalent compound: sugar is a covalent compound--it dissolves, but when it dissolves, it doesn't actually break up into its individual atoms.0650

It just dissolves: the crystal comes apart--the molecules separate.0661

Ionic compounds are different; so, when ionic compounds dissolve, they dissociate; in other words, they separate into their ions; so we must account for the total number of dissolved particles--that is what is important: the total number of free particles.0665

For example, if I had some magnesium chloride that I dropped into water, well, I have: 1 mole of magnesium chloride produces 1 mole of magnesium ions, plus 2 moles of chloride ions.0713

So, I have to account for...whatever the number of moles is that I get of that, it is actually 3 times that many particles.0727

1 mole of magnesium chloride produces 3 moles of free-flowing particles--of free particles--so it's actually 3 that is what I use when I calculate the mole fraction, OK?0737

That is it; that is the only thing that is different--you have to differentiate between ionic compounds and covalent compounds by accounting for the number of free particles that are floating around.0751

Let's do an example.0761

This is going to be Example #2.0765

OK, we have: 40.0 grams of solid potassium sulfate is dissolved (let's actually write it so we can read it; that might be nice) in 180.0 grams of water.0770

So, this time, they went ahead and they gave you the mass of the water directly, instead of volume--not a big deal.0796

OK, what is the vapor pressure of solution?0802

OK, well, again, we are going to use Raoult's Law; so, since I don't have it on this page, let me write it one more time.0812

The vapor pressure of solution is equal to the mole fraction of solvent, times the initial vapor pressure of solvent.0819

OK, well, we have the vapor pressure of solvent; that is going to end up being...it looks like this is going to be...I'm sorry, I didn't specify: this is 25 degrees Celsius, so we are going to use the 23.46; that is water.0830

The initial of the solvent is going to be 23.76 torr; so that is that one.0842

We need to find the mole fraction of the solvent; OK.0856

Well, let's find the number of moles of water; so moles of H2O: we have 180.0 grams; 1 mole is 18 grams, 18.0 grams; so we are looking at 10 moles of water.0859

OK, now let's find the number of moles of K2SO4, potassium sulfate.0876

Well, we have 40 grams of the potassium sulfate; and we want to do 1 mole of it; when we check the molar mass using a periodic table, we get 174.2 grams (I hope I did the arithmetic correctly--if not, not a problem--it's just a number), equals 0.2296 moles.0882

OK, now here is where we have to be careful: K2SO4...when K2SO4 dissociates, it produces 2 moles of potassium ions, plus 1 mole of sulfate ion.0905

1 mole of potassium sulfate produces 3 moles of particles--3 moles of free particles.0919

That is what matters: the identity of the species don't matter; these are colligative properties--these are...what matters is the number of particles that are floating around in solution.0930

The more number of particles you have floating around in solution, the more they get in the way of the solvent doing what it needs to do, which is escape into the vapor phase.0940

3 moles of free particles are formed.0949

So, when we do our mole fraction, our mole fraction is going to look like this.0954

The mole fraction of H2O is equal to...well, 10 moles of H2 over 10 plus three times the .2296 (right? .2296 is the number of moles of potassium sulfate, times 3 because, for every mole of potassium sulfate, three moles of free particles are going to be floating around in that solution).0962

So, you get: 0.9356; therefore, the vapor pressure of solution is equal to 0.9356 (let me make the numbers a little bit bigger; I don't know why--I usually have a habit of doing big numbers, and lately I know I have been doing small numbers), times 23.76 torricelli, which gives us 22.23 torr.0986

There you go: the only difference--handle it exactly the same way, but when you are dealing with an ionic compound, make sure you account for the dissociation of the ion and the number of free particles that are floating around--very important.1023

OK, so the identity of the dissolved species doesn't matter, just how many; it doesn't matter if it's sucrose or potassium sulfate or whatever.1035

It is how many particles, not the identity--just like gases, remember?--the identity of the gas doesn't matter--1 mole of gas at standard temperature and pressure always occupies 22.4 liters.1043

All gases--it doesn't matter what the identity of the gas is; what matters is the number of particles.1055

OK, so now, let's discuss non-ideal solutions.1063

What we have been discussing are ideal solutions; now, we will discuss non-ideal solutions.1066

This is analogous to discussing the non-ideal gas law versus the ideal gas law: the ideal gas law can be...actually, for most purposes, it's just fine; and Raoult's Law, for most purposes, is actually just fine.1075

But this is an experimental science--it is chemistry--so when we do the experiment, it doesn't always fit with the theory, with the numbers, and we need to actually explain why that is the case.1088

So, let's explain why.1099

OK, so: so far (well, you know what, I'm not going to write this part out), what we have assumed is that the solute is non-volatile--that is some solid crystal that you drop in the water; you mix it up; you dissolve it; it's non-volatile.1102

In other words, the solute itself that you put in the solvent doesn't have a vapor pressure of its own.1115

But, if you mix a liquid and a liquid (like methanol in water, or hexane in benzene, or sodium acetate in pentane--something like that), it is a liquid-liquid.1122

Well, all liquids have a certain vapor pressure; so now, when you mix a liquid and a liquid, it is still just a solution; you have some liquid that you are putting into another liquid, some solute that you are putting into a solvent.1142

Now, both of those liquids--the molecules can escape into the vapor phase.1155

The vapor pressure of solution is now a sum of the mole fractions of each, times the vapor pressures of each.1162

Let's see--so non-ideal solutions: for liquid-liquid solutions, where both are volatile, Raoult's Law becomes: the vapor pressure of solution is equal to the mole fraction of A, times the vapor pressure of A (pure A), plus the mole fraction of B, times the vapor pressure of pure B.1171

That is it: we are just sort of combining the Raoult's Law for the individual liquids, but now we are mixing both liquids, so we have to account for both of their partial pressures.1222

The total pressure of the solution--the total number of molecules of vapor--some of the vapor molecules are going to be of A; some of the molecules are going to be of B; each one of them contributes to the total pressure (the total number of particles above the liquid at a given temperature).1233

OK, so let me draw this out so you see what is going on.1248

What I am going to draw is an ideal situation: so under ideal conditions, this is what we would expect; this is the kind of behavior we would expect.1255

Let me go back to blue.1263

Now, I'm going to go from here; I'm going to go up to here; then, I'm going to go here; I'm going to go down this way, and I'll...the mole fraction of A increases as we move in this direction; the mole fraction of B increases as we move in this direction.1265

Therefore, at this point, this is pure B; and at this point, we have pure A, right?1285

So, if we start with absolutely no A and pure B, well, that is what this represents.1295

As we add more A, less B, more A, less B...this here represents the mixture, if you will: a certain amount of B, a certain amount of A; a certain amount of B, a certain amount of A; a certain amount of B, a certain amount of A; that is all this is.1301

OK, and they are represented by mole fraction: as mole fraction goes from 0 to 1...well, for pure A, when it's 1, it is pure A; when the mole fraction of B is 1, it's pure B.1320

There is any other combination; so if you want to draw vertical lines, that just represents how much B we have and how much A we have in a given solution.1331

Well, the vapor pressure is going to look like this.1339

It is going to be this number, plus that number.1349

Again, you are just adding graphs; that is all that is happening here.1352

It is this number plus that number, and you are going to get this number; so this actually, down here, doesn't really matter all that much; what we want you to realize is that the vapor pressure of the solution is the sum of the mole fractions of each, times the standard vapor pressure of that liquid alone.1356

That is what this is saying: you are just adding two functions to get a final function.1376

You have been doing this for years in your precalculus and your algebra classes, so it shouldn't be a problem.1380

Now, this is ideal behavior right here.1385

In other words, all we have done is take 2 things that are volatile and added them together.1394

This is what should happen--what we expect to happen, theoretically.1399

OK, when the two liquids are very much alike, this happens--when the two liquids are very much alike.1403

What we mean by "very much alike": we mean they have similar properties and similar structures--"very much alike."1415

So, for example, if you had something like water and ethanol: ethanol is just regular alcohol--the alcohol that you drink; the structures of those two are actually very, very similar, and because they are very, very similar, they are actually going to behave in an ideal fashion.1422

Now, we will talk about how, actually, it deviates from ideal behavior; but any time you put two liquids together--when you mix two liquids to make a solution--if the two liquids have a lot of things in common (a lot of properties, and are very much alike structurally), what you are going to get is ideal behavior.1441

In other words, your vapor pressure of solution is going to equal this right here.1459

Now, let's talk about deviation from ideal behavior.1464

There are two ways to deviate from ideal behavior: there is something called negative deviation, and what that means is: when the two liquids have a special affinity for each other, such as hydrogen bonding (and more often than not, it is going to be hydrogen bonding that sort of creates the negative deviation), the Psolution measured is lower than expected by Raoult's Law.1468

So, the equation that I just gave--that will give you an expected vapor pressure, but because the two liquids have a special affinity for each other (for example, water and ethanol--there is hydrogen bonding that takes place between those two)--because of that, the vapor pressure that we measure is going to be less than what we calculate by this law.1560

That is negative deviation, and what this looks like is the following.1582

I'm going to draw the same graph that I had...well, not graph--the same diagram that I had on the previous page.1588

And so, let me go this way, except--notice that I have reversed the colors this time.1595

I have one going that way; so this is...that would be ideal behavior; negative deviation looks like this.1600

This is lower; this is lower than expected; therefore, this is going to be lower than expected.1615

Let me go over that one in black.1625

Don't worry so much about these; this is the one that I am concerned about.1633

Ideal behavior would be right there: this is what the equation that I just gave you would predict.1636

However, because these things actually have a greater affinity for each other (in this case, hydrogen bonding--for example, hydrogen bonding), the vapor pressure that we measure is less than what we expect or calculate from this equation.1641

This is called negative deviation, and again, it makes perfect sense.1655

If you have two liquids that you would expect to just sort of treat...one liquid mixes with another liquid, so you just add up their mole fractions times their standard vapor pressures, and you should get a number; that number should be somewhere on that line, depending on the relative amounts of each liquid that you use.1659

However, because of the hydrogen bonding, this ethanol and this water actually are attracted to each other more; therefore, they will not let go of each other all that much so that they can go off into the vapor phase.1678

You actually need more energy to make that happen; but at a given temperature, the energy is fixed; therefore, the vapor pressure will actually be lower than you expect.1689

That is all that it is saying; it is saying that, when you measure a vapor pressure that is lower than you expect from calculation, that means it's a negative deviation--that means the two liquids have an extra-special affinity for each other.1700

That means they want to be together--they like being together.1712

The opposite of this is positive deviation.1716

Oh, let me give you an example of this one; so, for example, if I mix acetone (which has a molecular structure like this--wow, you know what, I like black--I think I'll stick with that) and water--if you mix acetone and water, well, there is some serious hydrogen bonding (let me draw it another way, so you can actually see the hydrogen bonding): this is going to be H; this is going to be O; this is going to be H.1718

There is hydrogen bonding; because of that hydrogen bonding, the acetone and the water are actually more attracted to each other; therefore, the vapor pressure we measure of their mixture is less than what we would expect: negative deviation.1746

OK, now let's do positive deviation.1759

Positive deviation is the opposite: it is when the two liquids' interactions are weaker than the solvents alone--weaker than the solvent and solute alone.1765

So, for example, if I had hexane--pure hexane--the hexane molecules interact with each other.1802

If I had water, the water molecules interact with each other.1808

If I put hexane and water together, hexane and water are not very much alike; in fact, they do not like to be together (you know this: oil and water--they don't mix).1811

Hexane is just a smaller version of oil, if you will--it's a hydrocarbon, not polar...and we will talk about what polar means; but water and hexane are not very much alike; they don't like to be together.1819

Therefore, they actually, literally, want to be apart; because they want to be apart, it is more likely that they will push away from each other and actually go into the vapor phase sooner, because they don't like being together.1831

Whereas, up here, these molecules that have a special affinity do like being together; so a positive deviation (if we stick to this graph, I'm going to do the positive deviation in blue)--what the Raoult's Law equation says for a given concentration--I should be here; but when I measure the vapor pressure, there is actually more vapor above the liquid.1845

What that means is that the molecules, mixed together--they don't want to be together, so they actually will go out of their way to escape into the vapor phase to avoid being so close together in the liquid form.1876

The vapor pressure is actually up here: the measured is higher than what I expect.1888

This is called positive deviation.1893

I'll let you think about that a little bit, and I will finish off with an example here.1896

Let's do this in black; so we have Example 3.1901

5.8 grams of acetone is mixed with 12 grams of CHCl3; OK, now, at 35 degrees Celsius, the measured vapor pressure of solution is equal to 265 torr.1909

OK, is this an ideal solution?1949

In other words, does it actually obey Raoult's Law?1958

Well, let's use Raoult's Law, calculate what we expect, compare it to what we measured (which is 265 torr), and see if it is lower or higher than that.1961

If it's lower than that, it's negative deviation; if it's higher than that, it's positive deviation; in either case, it's a non-ideal solution.1969

If it is close to 265 (you know, in the 260 to 270 range), it's an ideal solution.1976

OK, so our ideal is: solution equals the mole fraction of acetone (I'll just call it A...yes, that is fine), times the normal vapor pressure of acetone, plus the mole fraction of (I'll call this...I'll just do CHCl3...here we go again: chemistry with all of its symbolism, all over the place).1982

OK, so let's calculate the number of moles of CHCl3.2014

We have 12 grams, and 1 mole of that is actually equal to 119.4, equals 0.1005 mol.2021

And then, moles of C3H6O (that is the acetone): we have 5.8 grams, times 1 mole, which is 58.1 grams; OK, and we get 0.0998 mol.2037

Therefore, the mole fraction of acetone is equal to 0.0998, divided by 0.1005 plus 0.0998; you end up with 0.5.2056

And the mole fraction of the CHCl3 is equal to 0.1005, divided by 0.1005, plus 0.0998; and you actually end up with, again, .5.2076

So you see that the mole fraction of each is .5.2093

Now, our P solution is equal to the mole fraction of A (0.5), times its vapor pressure of the pure solvent at that temperature.2097

In the case of acetone at 35 degrees Celsius, it is 293 torr.2115

That is information that is actually given to you, or you can look it up.2120

...plus 0.5, which is the mole fraction of the CHCl3, and its vapor pressure (35 degrees Celsius, pure solvent) is 345 torr--that is going to equal 319 torr.2124

So, what I would expect under normal circumstances, without accounting for affinity or disaffinity, is 319 torr.2140

Well, what I measured was 293 torr; clearly, 293 torr is less than 319 torr, so this is negative deviation.2148

Negative deviation means that the acetone and the CHCl3 have some sort of an extra affinity to each other.2158

Well, let's see what that affinity is.2165

As it turns out, it is going to be exactly what you think: hydrogen bonding.2167

This is acetone; this is the H; this extra bonding--the hydrogen bonding--this intermolecular force between the acetone and the CHCl3--causes them to actually stick together more than they normally would.2173

Because they stick together more than they normally would, there are fewer molecules jumping out of solution into the vapor phase.2195

Because there are fewer molecules in the vapor phase, the vapor pressure that I measured is lower than what I expected.2204

That is what is going on; so that is it--standard Raoult's Law; I think the equation is pretty simple, and hopefully you understand what it is that is going on.2211

It is just: when you mix things, because now you don't have a pure solvent--you have other particles floating around in solution--they are actually getting in the way of the solvent particles from reaching the surface in order to break out into the vapor phase.2221

That is all that is going on: if you understand that physically, you will understand everything else.2234

Thank you for joining us here at Educator.com.2239

We'll see you next time; goodbye.2241