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Throughout our journey through chemistry so farŁŹ
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we've touched on the interactions between molecules,
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metal molecules,
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how they attract each other
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because of the sea of electrons and water molecules.
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But I think about it's good to have a general discussion
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all of the different types of molecular interactions
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and what it means for the boiling points
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or the melting points of a substance.
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So I'll start with the weakest.
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Let's say I had a bunch of helium.
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Helium, you know, I'll just draw it as helium atoms.
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We'll look in the Periodic Table,
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and what I'm going to do now with helium
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I could do with any of the noble gases.
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Because the point is that noble gases are happy.
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Their outer orbital is filled.
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Let's say, neon or helium --let me do neon,actually,
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because neon has a full eight in its orbital
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so we could write neon like neon
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and it's completely happy.
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It's completely satisfied with itself.
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And so in a world where it's completely satisfied,
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there's no obvious reason just yet
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-- I'm going to touch on a reason why it should be
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-- if these electrons are evenly distributed
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around these atoms,
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then these are completely neutral atoms.
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They don't want
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to bond with each other or do anything else,
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so they should just float around
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and there's no reason for them
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to be attracted to each other
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or not attracted to each other.
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But it turns out that
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neon does have a liquid state,
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if you get cold enough,
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and so the fact that it has a liquid state
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means that there must be some force
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that's making the neon atoms attracted to each other,
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some force out there.
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Because it's in a very cold state,
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because for the most part,
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there is not a lot of force that attracts them
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so it'll be a gas at most temperatures.
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But if you get really cold,
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you can get a very weak force
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that starts to connect
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or makes the neon molecules want
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to get towards each other.
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And that force comes out of the reality
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that we talked about early on
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that electrons are not in a fixed,
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uniform orbit around things.
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They're probablistic.
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And if we imagine, let me say neon now,
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instead of drawing
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these nice and neat valence dot electrons like that,
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instead, I can kind of draw its electrons as
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-- it's a probability cloud and
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it's what neon's atomic configuration is.
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1s2 and it's outer orbital is 2s2 2p6, right?
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So it's highest energy electron,
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so, you know, it'll look-- I don't know.
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It has the 2s shell.
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The 1s shell is inside of that
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and it has the p-orbitals.
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The p-orbitals look like that in different dimensions.
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That's not the point.
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And then you have another neon atom
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and these are--
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and I'm just drawing the probability distribution.
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I'm not trying to draw a rabbit.
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But I think you get the point.
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Watch the electron configuration videos
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if you want more on this,
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but the idea behind these probability distributions
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is that the electrons could be anywhere.
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There could be a moment in time
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when all the electrons out over here.
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There could be a moment in time
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where all the electrons are over here.
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Same thing for this neon atom.
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If you think about it,
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out of all of the possible configurations,
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let's say we have these two neon atoms,
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there's actually a very low likelihood
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that they're going to be completely evenly distributed.
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There's many more scenarios
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where the electron distribution
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is a little uneven in one neon atom or another.
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So if in this neon atom,
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temporarily its eight valence electrons
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just happen to be like, you know,
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one, two, three, four, five, six, seven,eight,
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then what does this neon atom look like?
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It temporarily has a slight charge in this direction, right?
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It'll feel like this side is more negative than this side
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or this side is more positive than that side.
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Similarly, if at that very same moment
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I had another neon
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that has 1 2 3 4 5 6 7 8...
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that had a similar-- actually, let me do that differently.
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Let's say that this neon atom is like this:
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one, two, three,four, five, six, seven, eight.
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So here, and I'll do it in a dark color
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because it's a very faint force.
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So this would be a little negative.
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Temporarly, just for that single moment in time,
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this will be kind of negative.
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That'll be positive.
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This side will be negative.
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This side will be positive.
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So you're going to have a little bit of an attraction
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for that very small moment of time
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between this neon and this neon,
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and then it'll disappear,
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because the electrons will reconfigure.
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But the important thing to realize is
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that almost at no point is neon's electrons
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going to be completely distributed.
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So as long as there's always
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going to be this haphazar distribution,
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there's always going to be
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a little bit of a--
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I don't want to say polar behavior,
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because that's almost too strong of a word.
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But there will always be
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a little bit of an extra charge
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on one side or the other side of an atom,
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which will allow it to attract it
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to the opposite side charges of
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other similarly imbalanced molecules.
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And this is a very, very, very weak force.
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It's called the London dispersion force.
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I think the guy who came up with this,
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Fritz London, who was neither--
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well, he was not British.
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I think he was German-American.
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London dispersion force,
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and it's the weakest of the van der Waals forces.
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I'm sure I'm not pronouncing it correctly.
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And the van der Waals forces are
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the class of all of the intermolecular,
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and in this case, neon-- the molecule, is an atom .
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It's just a one-atom molecule,
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I guess you could say.
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The van der Waals forces are
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the class of all of the intermolecular forces
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that are not covalent bonds
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and that aren't ionic bonds like we have in salts,
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and we'll touch on those in a second.
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And the weakest of them are
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the London dispersion forces.
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So neon, these noble gases,
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actually, all of these noble gases right here,
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the only thing that they experience
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are London dispersion forces,
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which are the weakest of
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all of the intermolecular forces.
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And because of that,
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it takes very little energy
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to get them into a gaseous state.
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So at a very, very low temperature,
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the noble gases will turn into the gaseous state.
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That's why they're called noble gases, first of all.
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And they're the most likely to behave like ideal gases
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because they have very,
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very small attraction to each other.
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Fair enough.
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Now, what happens when we go to situations
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when we go to molecules that have better attractions
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or that are a little bit more polar?
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Let's say I had hydrogen chloride, right?
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Hydrogen, it's a little bit ambivalent
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about whether or not it keeps its electrons.
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Chloride wants to keep the electrons.
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Chloride's quite electronegative.
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It's less electronegative than these guys right here.
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These are kind of the super-duper electron hogs,
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nitrogen, oxygen, and fluorine,
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but chlorine is pretty electronegative.
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So if I have hydrogen chloride,
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so I have the chlorine atom right here,
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it has seven electrons
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and then it shares an electron with the hydrogen.
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It shares an electron with the hydrogen,
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and I'll just do it like that.
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Because this is a good bit more
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electronegative than hydrogen,
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the electrons spend a lot of time out here.
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So what you end up having is
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a partial negative charge on the side,
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where the electron hog is,
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and a partial positive side.
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And this is actually
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very analogous to the hydrogen bonds.
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Hydrogen bonds are actually a class of this type of bond,
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which is called a dipole bond,
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or dipole-dipole interaction.
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So if I have one chlorine atom like that
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and if I have another chlorine atom,
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the other chlorin eatoms looks like this.
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If I have the other chlorine atom--
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let me copy and paste it--
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right there,
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then you'll have this attraction between them.
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You'll have this attraction
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between these two chlorine atoms--
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oh, sorry, between these
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two hydrogen chloride molecules.
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And the positive side,
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the positive pole of this dipole
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is the hydrogen side,
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because the electrons have kind of left it,
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will be attracted to the chlorine side
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of the other molecules.
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And because this van der Waals force,
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this dipole-dipole interaction
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is stronger than a London dispersion force.
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And just to be clear,
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London dispersion forces occur in
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all molecular interactions.
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It's just that it's very weak
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when you compare it to pretty much anything else.
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It only becomes relevant
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when you talk about things with noble gases.
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Even here, they're also London dispersion forces
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when the electron distribution
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just happens to go one way or the other
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for a single instant of time.
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But this dipole-dipole interaction is much stronger.
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And because it's much stronger,
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hydrogen chloride is
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going to take more energy to,
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get into the liquid state,
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or even more, get into the gaseous state than,
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say, just a sample of helium gas.
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Now, when you get even more electronegative,
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when this guy's even more electronegative
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when you're dealing with nitrogen, oxygen or fluorine,
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you get into a special case of
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dipole-dipole interactions,
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and that's the hydrogen bond.
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So it's really the same thing if
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you have hydrogen fluoride,
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a bunch of hydrogen fluorides around the place.
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Maybe I could write fluoride,
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and I'll write hydrogen fluoride here.
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Fluoride its ultra-electronegative.
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It's one of the three most electronegative atoms
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on the Periodic Table,
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and so it pretty much hogs all of the electrons.
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So this is a super-strong case of
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the dipole-dipole interaction,
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where here, all of the electrons are going to
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be hogged around the fluorine side.
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So you're going to have
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a partial positive charge,
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positive, partial negative,
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partial positive, partial negative and so on.
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So you're going to have this,
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which is really a dipole interaction.
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But it's a very strong dipole interaction,
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so people call it a hydrogen bond
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because it's dealing with
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hydrogen and a very electronegative atom,
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where the electronegative atom
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is pretty much hogging all of
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hydrogen's one electron.
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So hydrogen is sitting out here with just a proton,
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so it's going to be pretty positive,
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and it's really attracted to
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the negative side of these molecules.
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But hydrogen,
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all of these are van der Waals.
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So van der Waals, the weakest is London dispersion.
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Then if you have a molecule
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with a more electronegative atom,
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then you start having a dipole
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where you have one side where molecule becomes polar
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and you have the interaction
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00:10:31,330 --> 00:10:32,470
between the positive and the negative side of the pole.
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It gets a dipole-dipole interaction.
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And then an even stronger type of bond
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is a hydrogen bond
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because the super-electronegative atom
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is essentially stripping off
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the electron of the hydrogen,
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or almost stripping it off.
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It's still shared,
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but it's all on that side of the molecule.
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Since this is even a stronger bond between molecules,
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it will have even a higher boiling point.
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So London dispersion,
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and you have dipole or polar bonds,
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and then you have hydrogen bonds.
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All of these are van der Waals
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but because the strength of
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the intermolecular bond gets stronger,
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boiling point goes up
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because it takes more and more energy to
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separate these from each other.
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In the next video-- i realize I'm out of time.
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So this is a good survey, I think,
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of just the different types of
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intermolecular interactions
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that aren't necessarily covalent or ionic.
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In the next video,
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I'll talk about some of the covalent and ionic types of
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structures that can be formed
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and how that might affect the different boiling points.