Metallic Bonding
Summary
TLDRIn this chemistry essentials video, Mr. Andersen explains metallic bonding through the electron sea model, where delocalized electrons are shared among metal atoms. This model accounts for metals' conductivity, malleability, ductility, and low volatility. However, the shell model is necessary to understand anomalies in melting points across transition metals. The video explores how electron configurations, particularly unpaired electrons in d orbitals, affect these properties, with a focus on the transition from high to low melting points as electrons fill and pair in the d subshells.
Takeaways
- π¬ Metallic bonding involves a number of atoms sharing their electrons, forming a 'sea of electrons'.
- π The electron sea model is the primary way to visualize metallic bonding, where electrons are delocalized and free to move.
- β‘ Metals exhibit high conductivity due to the presence of free electrons that can easily flow through the material.
- π¨ Malleability in metals is explained by the electron sea model, allowing atoms to slide past each other when hammered.
- π© Ductility is the property of metals to stretch rather than break when pulled, due to the freedom of atoms to move around each other.
- π₯ Metals have low volatility, which means they have high melting and boiling points, attributed to the strong attraction between the sea of electrons and the positive charges in the nucleus.
- π The electron sea model does not fully explain the variation in melting points across transition metals, necessitating the shell model for a complete understanding.
- π The shell model becomes important when discussing the electron configurations of transition metals, especially to explain anomalies in melting points.
- π The electron configurations of transition metals often involve unpaired electrons in d orbitals, contributing to their metallic properties.
- π The melting point of transition metals does not consistently increase with the number of electrons; it can dip, as seen with chromium, due to its unique electron configuration.
- π« As we move towards nonmetals, like zinc, the properties of metals start to change, showing a deviation from typical metallic behavior.
Q & A
What is the electron sea model in the context of metallic bonding?
-The electron sea model is a way to visualize metallic bonding where electrons are delocalized and shared among a number of atoms, creating a 'sea' of electrons that are free to move within the structure of the metal.
Why can't there be just one metallic bond?
-Metallic bonds involve a collective sharing of electrons among multiple atoms, so there must be a group of atoms to form this type of bond, not just one.
What properties of metals does the electron sea model account for?
-The electron sea model accounts for properties such as conductivity, malleability, ductility, and low volatility of metals.
How does the electron sea model explain the conductivity of metals?
-In the electron sea model, the free electrons can easily flow through the metal, which allows for the conduction of electricity and heat.
What does malleability mean in terms of metals?
-Malleability refers to the property of metals that allows them to be hammered or rolled into thin sheets without breaking, due to the smooth sliding of atoms in the metallic bond.
What is ductility, and how does it relate to metallic bonding?
-Ductility is the property of metals that enables them to be stretched into wires without breaking. It is related to metallic bonding because the atoms have the freedom to move around each other, allowing the metal to stretch rather than fracture.
Why do metals have low volatility?
-Metals have low volatility because of the strong electrostatic attraction between the positively charged protons and the delocalized negatively charged electrons, making it difficult to separate the atoms and turn the metal into a liquid or gas.
How does the electron sea model relate to the melting point of metals?
-The electron sea model suggests that metals with more free electrons should have higher melting points due to the stronger electrostatic attraction. However, this is not always the case, and the shell model is sometimes needed to explain variations in melting points.
What is the significance of unpaired electrons in transition metals?
-Unpaired electrons in transition metals contribute to the properties of metals by allowing for greater freedom of movement of electrons within the electron sea, which is essential for metallic bonding and the associated properties.
Why does the melting point of metals not consistently increase as you move across the transition metals?
-The melting point of metals does not consistently increase across the transition metals because factors such as electron configuration and the stability of the electron shell structure can influence the melting point more than just the number of valence electrons.
What is the difference between the electron sea model and the shell model in explaining metallic bonding?
-The electron sea model focuses on the delocalized electrons shared among metal atoms, while the shell model delves into the specific electron configurations within the atoms, which can help explain phenomena like variations in melting points that the electron sea model cannot account for.
Outlines
π¬ Metallic Bonding and Electron Sea Model
Mr. Andersen introduces the concept of metallic bonding in this chemistry essentials video, emphasizing that it involves a collective sharing of electrons among multiple atoms, forming a 'sea of electrons.' This electron sea model is key to understanding metals' properties such as conductivity, malleability, ductility, and low volatility. The video explains how the delocalized electrons provide metals with the ability to conduct electricity and heat, and how the atoms' freedom to move allows for malleability and ductility. The electron sea also contributes to metals' high melting and boiling points due to the strong attractive forces between the positive and negative charges. The video hints at the need for the shell model to explain variations in melting points across different transition metals.
π Electron Configurations and Melting Points in Transition Metals
This paragraph delves into the relationship between electron configurations and the melting points of transition metals. It discusses how adding electrons to the valence shell generally increases the melting point due to the increased electrostatic attraction. However, the pattern is disrupted when the 4s subshell is filled before the 3d subshell, as seen with chromium, leading to a dip in melting point. The video highlights the importance of electron pairing in affecting the properties of metals, noting that paired electrons reduce the number of free electrons available for conductivity and other metallic properties. The summary of electron configurations from scandium to zinc illustrates the transition from metals to nonmetals and the corresponding change in properties, concluding with the observation that metallic bonding can be understood through the delocalized electron model to predict macroscopic properties of metals.
Mindmap
Keywords
π‘Metallic Bonding
π‘Electron Sea Model
π‘Delocalized Electrons
π‘Conductivity
π‘Malleability
π‘Ductility
π‘Low Volatility
π‘Melting Point
π‘Shell Model
π‘Transition Metals
π‘Electron Configurations
Highlights
Understanding that you can't have one metallic bond; you need a number of atoms together sharing their electrons.
Metallic bonding is visualized through the electron sea model, where electrons are shared by all the atoms, creating a sea of electrons.
In metallic bonding, we have delocalized electrons that have the freedom to move.
The electron sea model accounts for the properties of metals, such as conductivity, malleability, ductility, and low volatility.
Sometimes, the shell model is needed to explain phenomena like melting points in metallic bonding.
Positive charges of protons are held inside the sea of negative charge electrons, which are constantly in motion.
Transition metals, which have a lot of unpaired electrons in their d orbital, are a key focus in metallic bonding.
Metals are good at conducting electricity and heat because of the free electrons that can flow easily.
Metals are malleable, meaning they can be flattened out without breaking, a property used by blacksmiths to create gold leaf.
Metals show ductility, meaning they can stretch rather than break when pulled, unlike brittle materials.
Metals have low volatility, resulting in high melting and boiling points due to the strong attraction between positive and negative charges.
The electron sea model explains properties well, but the shell model is needed to explain the melting point trend across transition metals.
Melting points increase across the period but show a dip at chromium due to electron configurations.
The melting point pattern picks up again after magnesium, where electrons start pairing, leading to lower melting points towards zinc.
Understanding the delocalized electron model helps predict macroscopic properties of metals like conductivity, malleability, ductility, and low volatility.
Transcripts
Hi. It's Mr. Andersen and this is chemistry essentials video 21. It's on metallic bonding.
And it's important that you understand that you can't have one metallic bond. You have
to have a number of atoms together sharing their electrons. And therefore sharing their
bonding. And so the way we look at metallic bonding is the electron sea model where you
have all of these electrons. And they're shared by all the atoms. It creates a sea of electrons.
And then the protons are kind of held on the inside of that. And so in metallic bonding
what we have are delocalized electrons. Or electrons that have the freedom to move. And
the way we visualize that is through this electron sea model. It accounts for a lot
of the properties of metals. Like their conductivity, malleability, ductility, low volatility. And
sometimes we have to go to the shell model however to explain new phenomena. And we'll
get to that when we're looking at melting point. And all of that has to do with bonding.
And so if we look at metallic bonding or these shared bonds between all the metals, visualize
it like this. We have the positive charges of the protons in the nucleus. And then we
have electrons that are free to go. They don't want to get too close to each other. Their
going to repel each other. And so what they do is they simply drift around. And they're
constantly in motion. And what you create is this sea of electrons that have a negative
charge. And then the protons are going to be held on the inside of that. And that's
the best way to visualize the metallic bonding. And remember these are going to be transition
metals. So these are going to be atoms that have a lot of unpaired electrons in their
d orbital. And as a result these electrons have a freedom to move. And as a result we
have all of these properties that come from metals. So number 1 they are very good at
conductivity. So that means conducting electricity and also conducting heat. And the reason why
is that electricity for example is simply the flow of electrons. And so if we have free
electrons it's easy for them to flow through that metal. Likewise with heat, since those
electrons and those atoms have a huge amount of freedom, we can move a lot of that energy
through the material. They also are incredibly malleable. And what malleable means is that
you can hit them and they are going to flatten out. And so if you're a blacksmith you're
using that property of heating up these atoms in the metallic bonds. And then as you hit
it you're able to slide them past one another. It's going to be smooth sliding. And that
explains how we could get something like gold leaf which is simply gold that we hit over
and over and over again until it's razor thin. They also show ductility. And what ductility
means is that it's ductile. Or that means that if we pull it, it's going to stretch
rather than break. And so if we were to test the tensile strength of different materials,
so what you do is you put them in a big vice like this. Then you simply pull on it. If
something is ductile what that means is as you pull on it it's going to stretch out before
it eventually breaks. If it's not, it's brittle. What it's going to do is simply break in half.
And metals show this. And the reason they show that is that all of these atoms have
freedom to move around each other. And so when you pull on each other it's going to
stretch it out. They also show low volatility. What that means is that they're going to have
a high melting point and a high boiling point. Why is that? Well think of all the positive
charges we have down in these metals. We have all of these negative charges. And so there's
going to be a huge attraction between the two. And so it's hard to pull off individual
ones to make them a liquid or eventually to make them a gas. And so you would think as
we move across the transition metals, so let's say we're going across this period from scandium
to zinc. As we move across we should be increasing the number of electrons. And so we should
be increasing something like this. Melting point. And it's not really right. And so let's
look at what the data looks like. So as we move across the period, it starts to go up
for awhile, but then it dips. And then it eventually goes down quite a bit. And so this
whole idea of an electron sea model works well. But when you get to something like this,
we have to start digging into the shell model to make sense of it. And so let's start by
looking at some electron configurations. So if we're looking at scandium it's going to
have 2 electrons in its 4s. And that's something interesting about transition metals. They're
valence electrons are actually going to be at a higher level but inside the s subshell.
Anyway, as we move across what we're doing is we're increasing the number of electrons.
So we're increasing the number of valence electrons. And so as we go to titanium and
then as we go to vanadium this all makes sense. If you can increase more of these electrons,
increase more of that charge, it's going to be harder to get this thing to melt. But if
you look here when we get to chromium, it kind of dips. And the reason why is that it
actually is not going to fill this 4s before it jumps into the 3d. And then as we go to
magnesium you get a real stable shell structure where all of these are filled. And so the
melting point is going to drop off. But now that pattern picks up again. Okay. Now we're
going to start adding electrons. So when we go to iron and cobalt and to nickel, now we're
adding these paired electrons. And as we pair those electrons, now we don't have those free
electrons anymore. And so we're going to decrease the melting point as we get all the way down
to zinc. And remember as we get to zinc we're moving over towards those nonmetals. And so
we're starting to see odd properties here as well. And so metallic bonding is pretty
simple. Did you learn to use a delocalized electron model to predict macroscopic properties
of metals? If you understand the sea model and you see how it affects conductivity, malleability,
ductility and low volatility, then you got it. And I hope that was helpful.
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