< Return to Video

Van Der Waals Forces

  • 0:01 - 0:03
    Throughout our journey through chemistry so farŁŹ
  • 0:03 - 0:06
    we've touched on the interactions between molecules,
  • 0:06 - 0:10
    metal molecules,
  • 0:10 - 0:11
    how they attract each other
  • 0:11 - 0:13
    because of the sea of electrons and water molecules.
  • 0:13 - 0:16
    But I think about it's good to have a general discussion
  • 0:16 - 0:19
    all of the different types of molecular interactions
  • 0:19 - 0:21
    and what it means for the boiling points
  • 0:21 - 0:23
    or the melting points of a substance.
  • 0:23 - 0:24
    So I'll start with the weakest.
  • 0:25 - 0:26
    Let's say I had a bunch of helium.
  • 0:26 - 0:30
    Helium, you know, I'll just draw it as helium atoms.
  • 0:30 - 0:32
    We'll look in the Periodic Table,
  • 0:32 - 0:34
    and what I'm going to do now with helium
  • 0:34 - 0:35
    I could do with any of the noble gases.
  • 0:35 - 0:38
    Because the point is that noble gases are happy.
  • 0:38 - 0:40
    Their outer orbital is filled.
  • 0:40 - 0:42
    Let's say, neon or helium --let me do neon,actually,
  • 0:42 - 0:45
    because neon has a full eight in its orbital
  • 0:45 - 0:46
    so we could write neon like neon
  • 0:46 - 0:49
    and it's completely happy.
  • 0:49 - 0:52
    It's completely satisfied with itself.
  • 0:52 - 0:57
    And so in a world where it's completely satisfied,
  • 0:57 - 1:00
    there's no obvious reason just yet
  • 1:00 - 1:02
    -- I'm going to touch on a reason why it should be
  • 1:02 - 1:03
    -- if these electrons are evenly distributed
  • 1:04 - 1:05
    around these atoms,
  • 1:05 - 1:06
    then these are completely neutral atoms.
  • 1:07 - 1:08
    They don't want
  • 1:08 - 1:09
    to bond with each other or do anything else,
  • 1:09 - 1:11
    so they should just float around
  • 1:11 - 1:12
    and there's no reason for them
  • 1:12 - 1:13
    to be attracted to each other
  • 1:13 - 1:15
    or not attracted to each other.
  • 1:15 - 1:16
    But it turns out that
  • 1:16 - 1:18
    neon does have a liquid state,
  • 1:18 - 1:20
    if you get cold enough,
  • 1:20 - 1:22
    and so the fact that it has a liquid state
  • 1:22 - 1:25
    means that there must be some force
  • 1:25 - 1:30
    that's making the neon atoms attracted to each other,
  • 1:30 - 1:31
    some force out there.
  • 1:31 - 1:33
    Because it's in a very cold state,
  • 1:33 - 1:34
    because for the most part,
  • 1:34 - 1:35
    there is not a lot of force that attracts them
  • 1:36 - 1:37
    so it'll be a gas at most temperatures.
  • 1:37 - 1:39
    But if you get really cold,
  • 1:39 - 1:41
    you can get a very weak force
  • 1:41 - 1:42
    that starts to connect
  • 1:42 - 1:44
    or makes the neon molecules want
  • 1:44 - 1:46
    to get towards each other.
  • 1:46 - 1:49
    And that force comes out of the reality
  • 1:49 - 1:50
    that we talked about early on
  • 1:50 - 1:53
    that electrons are not in a fixed,
  • 1:53 - 1:55
    uniform orbit around things.
  • 1:55 - 1:56
    They're probablistic.
  • 1:56 - 1:59
    And if we imagine, let me say neon now,
  • 1:59 - 2:00
    instead of drawing
  • 2:00 - 2:04
    these nice and neat valence dot electrons like that,
  • 2:04 - 2:07
    instead, I can kind of draw its electrons as
  • 2:07 - 2:09
    -- it's a probability cloud and
  • 2:09 - 2:12
    it's what neon's atomic configuration is.
  • 2:12 - 2:19
    1s2 and it's outer orbital is 2s2 2p6, right?
  • 2:19 - 2:20
    So it's highest energy electron,
  • 2:20 - 2:22
    so, you know, it'll look-- I don't know.
  • 2:22 - 2:24
    It has the 2s shell.
  • 2:24 - 2:26
    The 1s shell is inside of that
  • 2:26 - 2:28
    and it has the p-orbitals.
  • 2:28 - 2:32
    The p-orbitals look like that in different dimensions.
  • 2:32 - 2:33
    That's not the point.
  • 2:33 - 2:35
    And then you have another neon atom
  • 2:35 - 2:36
    and these are--
  • 2:36 - 2:39
    and I'm just drawing the probability distribution.
  • 2:39 - 2:40
    I'm not trying to draw a rabbit.
  • 2:40 - 2:42
    But I think you get the point.
  • 2:42 - 2:46
    Watch the electron configuration videos
  • 2:46 - 2:48
    if you want more on this,
  • 2:48 - 2:50
    but the idea behind these probability distributions
  • 2:50 - 2:53
    is that the electrons could be anywhere.
  • 2:53 - 2:55
    There could be a moment in time
  • 2:55 - 2:56
    when all the electrons out over here.
  • 2:56 - 2:57
    There could be a moment in time
  • 2:57 - 2:58
    where all the electrons are over here.
  • 2:58 - 2:59
    Same thing for this neon atom.
  • 2:59 - 3:01
    If you think about it,
  • 3:01 - 3:02
    out of all of the possible configurations,
  • 3:02 - 3:04
    let's say we have these two neon atoms,
  • 3:04 - 3:07
    there's actually a very low likelihood
  • 3:07 - 3:09
    that they're going to be completely evenly distributed.
  • 3:09 - 3:13
    There's many more scenarios
  • 3:13 - 3:14
    where the electron distribution
  • 3:14 - 3:16
    is a little uneven in one neon atom or another.
  • 3:17 - 3:18
    So if in this neon atom,
  • 3:18 - 3:21
    temporarily its eight valence electrons
  • 3:21 - 3:23
    just happen to be like, you know,
  • 3:24 - 3:28
    one, two, three, four, five, six, seven,eight,
  • 3:28 - 3:30
    then what does this neon atom look like?
  • 3:30 - 3:33
    It temporarily has a slight charge in this direction, right?
  • 3:33 - 3:37
    It'll feel like this side is more negative than this side
  • 3:37 - 3:39
    or this side is more positive than that side.
  • 3:39 - 3:44
    Similarly, if at that very same moment
  • 3:44 - 3:45
    I had another neon
  • 3:45 - 3:49
    that has 1 2 3 4 5 6 7 8...
  • 3:49 - 3:52
    that had a similar-- actually, let me do that differently.
  • 3:52 - 3:56
    Let's say that this neon atom is like this:
  • 3:56 - 4:01
    one, two, three,four, five, six, seven, eight.
  • 4:01 - 4:04
    So here, and I'll do it in a dark color
  • 4:04 - 4:06
    because it's a very faint force.
  • 4:06 - 4:07
    So this would be a little negative.
  • 4:07 - 4:09
    Temporarly, just for that single moment in time,
  • 4:09 - 4:11
    this will be kind of negative.
  • 4:11 - 4:12
    That'll be positive.
  • 4:12 - 4:14
    This side will be negative.
  • 4:14 - 4:16
    This side will be positive.
  • 4:16 - 4:18
    So you're going to have a little bit of an attraction
  • 4:18 - 4:21
    for that very small moment of time
  • 4:21 - 4:22
    between this neon and this neon,
  • 4:22 - 4:23
    and then it'll disappear,
  • 4:23 - 4:25
    because the electrons will reconfigure.
  • 4:25 - 4:27
    But the important thing to realize is
  • 4:27 - 4:31
    that almost at no point is neon's electrons
  • 4:31 - 4:32
    going to be completely distributed.
  • 4:32 - 4:34
    So as long as there's always
  • 4:34 - 4:35
    going to be this haphazar distribution,
  • 4:35 - 4:37
    there's always going to be
  • 4:37 - 4:39
    a little bit of a--
  • 4:39 - 4:41
    I don't want to say polar behavior,
  • 4:41 - 4:42
    because that's almost too strong of a word.
  • 4:42 - 4:44
    But there will always be
  • 4:44 - 4:46
    a little bit of an extra charge
  • 4:46 - 4:47
    on one side or the other side of an atom,
  • 4:47 - 4:49
    which will allow it to attract it
  • 4:49 - 4:50
    to the opposite side charges of
  • 4:50 - 4:53
    other similarly imbalanced molecules.
  • 4:53 - 4:56
    And this is a very, very, very weak force.
  • 4:56 - 4:58
    It's called the London dispersion force.
  • 4:58 - 5:01
    I think the guy who came up with this,
  • 5:01 - 5:03
    Fritz London, who was neither--
  • 5:03 - 5:05
    well, he was not British.
  • 5:05 - 5:07
    I think he was German-American.
  • 5:07 - 5:10
    London dispersion force,
  • 5:10 - 5:19
    and it's the weakest of the van der Waals forces.
  • 5:19 - 5:21
    I'm sure I'm not pronouncing it correctly.
  • 5:21 - 5:23
    And the van der Waals forces are
  • 5:23 - 5:25
    the class of all of the intermolecular,
  • 5:25 - 5:28
    and in this case, neon-- the molecule, is an atom .
  • 5:28 - 5:29
    It's just a one-atom molecule,
  • 5:29 - 5:30
    I guess you could say.
  • 5:30 - 5:32
    The van der Waals forces are
  • 5:32 - 5:34
    the class of all of the intermolecular forces
  • 5:34 - 5:36
    that are not covalent bonds
  • 5:36 - 5:38
    and that aren't ionic bonds like we have in salts,
  • 5:38 - 5:40
    and we'll touch on those in a second.
  • 5:40 - 5:41
    And the weakest of them are
  • 5:41 - 5:42
    the London dispersion forces.
  • 5:42 - 5:44
    So neon, these noble gases,
  • 5:44 - 5:47
    actually, all of these noble gases right here,
  • 5:47 - 5:48
    the only thing that they experience
  • 5:48 - 5:50
    are London dispersion forces,
  • 5:50 - 5:52
    which are the weakest of
  • 5:52 - 5:54
    all of the intermolecular forces.
  • 5:54 - 5:55
    And because of that,
  • 5:55 - 5:57
    it takes very little energy
  • 5:57 - 5:59
    to get them into a gaseous state.
  • 5:59 - 6:01
    So at a very, very low temperature,
  • 6:01 - 6:07
    the noble gases will turn into the gaseous state.
  • 6:07 - 6:10
    That's why they're called noble gases, first of all.
  • 6:10 - 6:14
    And they're the most likely to behave like ideal gases
  • 6:14 - 6:15
    because they have very,
  • 6:15 - 6:17
    very small attraction to each other.
  • 6:17 - 6:19
    Fair enough.
  • 6:19 - 6:21
    Now, what happens when we go to situations
  • 6:21 - 6:24
    when we go to molecules that have better attractions
  • 6:24 - 6:25
    or that are a little bit more polar?
  • 6:25 - 6:27
    Let's say I had hydrogen chloride, right?
  • 6:27 - 6:30
    Hydrogen, it's a little bit ambivalent
  • 6:30 - 6:32
    about whether or not it keeps its electrons.
  • 6:32 - 6:34
    Chloride wants to keep the electrons.
  • 6:34 - 6:37
    Chloride's quite electronegative.
  • 6:37 - 6:40
    It's less electronegative than these guys right here.
  • 6:40 - 6:43
    These are kind of the super-duper electron hogs,
  • 6:43 - 6:45
    nitrogen, oxygen, and fluorine,
  • 6:45 - 6:48
    but chlorine is pretty electronegative.
  • 6:48 - 6:50
    So if I have hydrogen chloride,
  • 6:50 - 6:53
    so I have the chlorine atom right here,
  • 6:53 - 6:56
    it has seven electrons
  • 6:56 - 6:59
    and then it shares an electron with the hydrogen.
  • 6:59 - 7:02
    It shares an electron with the hydrogen,
  • 7:02 - 7:03
    and I'll just do it like that.
  • 7:03 - 7:05
    Because this is a good bit more
  • 7:05 - 7:06
    electronegative than hydrogen,
  • 7:06 - 7:09
    the electrons spend a lot of time out here.
  • 7:09 - 7:11
    So what you end up having is
  • 7:11 - 7:13
    a partial negative charge on the side,
  • 7:13 - 7:15
    where the electron hog is,
  • 7:15 - 7:16
    and a partial positive side.
  • 7:16 - 7:18
    And this is actually
  • 7:18 - 7:20
    very analogous to the hydrogen bonds.
  • 7:20 - 7:23
    Hydrogen bonds are actually a class of this type of bond,
  • 7:23 - 7:24
    which is called a dipole bond,
  • 7:24 - 7:26
    or dipole-dipole interaction.
  • 7:26 - 7:28
    So if I have one chlorine atom like that
  • 7:28 - 7:30
    and if I have another chlorine atom,
  • 7:30 - 7:33
    the other chlorin eatoms looks like this.
  • 7:33 - 7:36
    If I have the other chlorine atom--
  • 7:36 - 7:38
    let me copy and paste it--
  • 7:38 - 7:39
    right there,
  • 7:39 - 7:43
    then you'll have this attraction between them.
  • 7:43 - 7:46
    You'll have this attraction
  • 7:46 - 7:48
    between these two chlorine atoms--
  • 7:48 - 7:49
    oh, sorry, between these
  • 7:49 - 7:52
    two hydrogen chloride molecules.
  • 7:52 - 7:53
    And the positive side,
  • 7:53 - 7:57
    the positive pole of this dipole
  • 7:57 - 7:58
    is the hydrogen side,
  • 7:58 - 8:00
    because the electrons have kind of left it,
  • 8:00 - 8:02
    will be attracted to the chlorine side
  • 8:02 - 8:04
    of the other molecules.
  • 8:04 - 8:06
    And because this van der Waals force,
  • 8:06 - 8:08
    this dipole-dipole interaction
  • 8:08 - 8:12
    is stronger than a London dispersion force.
  • 8:12 - 8:13
    And just to be clear,
  • 8:13 - 8:14
    London dispersion forces occur in
  • 8:14 - 8:16
    all molecular interactions.
  • 8:16 - 8:18
    It's just that it's very weak
  • 8:18 - 8:19
    when you compare it to pretty much anything else.
  • 8:19 - 8:21
    It only becomes relevant
  • 8:21 - 8:24
    when you talk about things with noble gases.
  • 8:24 - 8:26
    Even here, they're also London dispersion forces
  • 8:26 - 8:28
    when the electron distribution
  • 8:28 - 8:30
    just happens to go one way or the other
  • 8:30 - 8:31
    for a single instant of time.
  • 8:31 - 8:34
    But this dipole-dipole interaction is much stronger.
  • 8:34 - 8:36
    And because it's much stronger,
  • 8:36 - 8:38
    hydrogen chloride is
  • 8:38 - 8:39
    going to take more energy to,
  • 8:39 - 8:41
    get into the liquid state,
  • 8:41 - 8:44
    or even more, get into the gaseous state than,
  • 8:44 - 8:47
    say, just a sample of helium gas.
  • 8:47 - 8:50
    Now, when you get even more electronegative,
  • 8:50 - 8:51
    when this guy's even more electronegative
  • 8:51 - 8:54
    when you're dealing with nitrogen, oxygen or fluorine,
  • 8:54 - 8:56
    you get into a special case of
  • 8:56 - 8:58
    dipole-dipole interactions,
  • 8:58 - 9:00
    and that's the hydrogen bond.
  • 9:00 - 9:03
    So it's really the same thing if
  • 9:03 - 9:07
    you have hydrogen fluoride,
  • 9:07 - 9:12
    a bunch of hydrogen fluorides around the place.
  • 9:12 - 9:14
    Maybe I could write fluoride,
  • 9:14 - 9:17
    and I'll write hydrogen fluoride here.
  • 9:17 - 9:19
    Fluoride its ultra-electronegative.
  • 9:19 - 9:23
    It's one of the three most electronegative atoms
  • 9:23 - 9:24
    on the Periodic Table,
  • 9:24 - 9:29
    and so it pretty much hogs all of the electrons.
  • 9:30 - 9:34
    So this is a super-strong case of
  • 9:34 - 9:36
    the dipole-dipole interaction,
  • 9:36 - 9:38
    where here, all of the electrons are going to
  • 9:38 - 9:40
    be hogged around the fluorine side.
  • 9:40 - 9:41
    So you're going to have
  • 9:41 - 9:42
    a partial positive charge,
  • 9:42 - 9:43
    positive, partial negative,
  • 9:43 - 9:49
    partial positive, partial negative and so on.
  • 9:49 - 9:50
    So you're going to have this,
  • 9:50 - 9:54
    which is really a dipole interaction.
  • 9:54 - 9:56
    But it's a very strong dipole interaction,
  • 9:56 - 9:57
    so people call it a hydrogen bond
  • 9:57 - 9:59
    because it's dealing with
  • 9:59 - 10:01
    hydrogen and a very electronegative atom,
  • 10:01 - 10:03
    where the electronegative atom
  • 10:03 - 10:04
    is pretty much hogging all of
  • 10:04 - 10:06
    hydrogen's one electron.
  • 10:06 - 10:08
    So hydrogen is sitting out here with just a proton,
  • 10:08 - 10:09
    so it's going to be pretty positive,
  • 10:09 - 10:10
    and it's really attracted to
  • 10:10 - 10:12
    the negative side of these molecules.
  • 10:12 - 10:14
    But hydrogen,
  • 10:14 - 10:16
    all of these are van der Waals.
  • 10:16 - 10:19
    So van der Waals, the weakest is London dispersion.
  • 10:19 - 10:22
    Then if you have a molecule
  • 10:22 - 10:25
    with a more electronegative atom,
  • 10:25 - 10:26
    then you start having a dipole
  • 10:27 - 10:30
    where you have one side where molecule becomes polar
  • 10:30 - 10:32
    and you have the interaction
    404
    00:10:31,330 --> 00:10:32,470
    between the positive and the negative side of the pole.
  • 10:32 - 10:36
    It gets a dipole-dipole interaction.
  • 10:36 - 10:38
    And then an even stronger type of bond
  • 10:38 - 10:39
    is a hydrogen bond
  • 10:39 - 10:42
    because the super-electronegative atom
  • 10:42 - 10:43
    is essentially stripping off
  • 10:43 - 10:45
    the electron of the hydrogen,
  • 10:45 - 10:46
    or almost stripping it off.
  • 10:46 - 10:47
    It's still shared,
  • 10:47 - 10:49
    but it's all on that side of the molecule.
  • 10:49 - 10:52
    Since this is even a stronger bond between molecules,
  • 10:52 - 10:54
    it will have even a higher boiling point.
  • 10:54 - 10:57
    So London dispersion,
  • 10:57 - 11:01
    and you have dipole or polar bonds,
  • 11:01 - 11:04
    and then you have hydrogen bonds.
  • 11:04 - 11:08
    All of these are van der Waals
  • 11:08 - 11:10
    but because the strength of
  • 11:10 - 11:12
    the intermolecular bond gets stronger,
  • 11:12 - 11:16
    boiling point goes up
  • 11:16 - 11:19
    because it takes more and more energy to
  • 11:19 - 11:21
    separate these from each other.
  • 11:21 - 11:23
    In the next video-- i realize I'm out of time.
  • 11:23 - 11:25
    So this is a good survey, I think,
  • 11:26 - 11:27
    of just the different types of
  • 11:27 - 11:28
    intermolecular interactions
  • 11:28 - 11:30
    that aren't necessarily covalent or ionic.
  • 11:30 - 11:31
    In the next video,
  • 11:31 - 11:34
    I'll talk about some of the covalent and ionic types of
  • 11:34 - 11:35
    structures that can be formed
  • 11:35 - 11:38
    and how that might affect the different boiling points.
Title:
Van Der Waals Forces
Description:

Van Der Waals Forces: London Dispersion Forces, Dipole Attractions, and Hydrogen Bonds.

more » « less
Video Language:
English
Duration:
11:39
oliviagao8971 edited English, British subtitles for Van Der Waals Forces
oliviagao8971 added a translation

English, British subtitles

Revisions