Intermolecular Forces, Liquids, and Solids Lực liên kết liên phân tử Trạng thái ngưng kết của vật chất... Liquids and Solids: A Molecular ComparisonTính chất vật lý của các chất được hiể
Trang 1Intermolecular Forces,
Liquids, and Solids
Lực liên kết liên phân tử Trạng thái ngưng kết của vật chất
Trang 2Liquids and Solids: A Molecular Comparison
Tính chất vật lý của các chất được hiểu theo khái niệm của thuyết động học phân tử ( kinetic molecular theory ) như sau:
• Chất khí dễ bị nén, có hình dạng và thể tích của vật chứa
:
• Các phân tử chất khí cách xa nhau, không tương tác với nhau
• Chất lỏng hầu như không bị nén, có hình dạng (nhưng
không có thể tích) của vật chứa :
• Các phân tử chất lỏng được giữ gần nhau hơn các phân tử chất khí,
nhưng không chắc đến mức chúng không thể trượt qua nhau (slide past each other)
• Chất rắn không bị nén, có hình dạng và thể tích xác định
• Các phân tử chất rắn được giữ gần nhau Các phân tử chất rắn được
chắc đến mức chúng không thể trượt qua nhau được
Trang 3A Molecular Comparison of Liquids and Solids
Trang 4A Molecular Comparison of Liquids and Solids
• Converting a gas into a liquid or solid requires the molecules to get closer to each other/ Để biến đổi một chất khí thành lỏng hay rắn:
– cool or compress/ làm lạnh hay nén
• Converting a solid into a liquid or gas requires the molecules to move further apart:/Để biến đổi một chất rắn thành lỏng hay
khí:
– heat or reduce pressure/ gia nhiệt hay giảm áp suất
• The forces holding solids and liquids together are called
intermolecular forces ( lực giữ các chất lỏng và rắn lai với nhau
được gọi là lực liên phân tử).
Trang 5Intermolecular Forces
• The covalent bond holding a molecule together is an
intramolecular forces (lục nội phân tử)
• The attraction between molecules is an intermolecular force (lực liên phân tử)
• Intermolecular forces are much weaker than
intramolecular forces (e.g 16 kJ/mol vs 431 kJ/mol for HCl).
• When a substance melts (nóng chảy) or boils (sôi) the
intermolecular forces are broken (not the covalent
bonds).
• When a substance condenses (ngưng tụ)
Trang 6Intermolecular Forces
Trang 7Intermolecular Forces
Ion-Dipole Forces ( l ực ion-lưỡng cực)
• Interaction between an ion (e.g Na+) and a dipole (e.g water).
• Strongest of all intermolecular forces:
– Since Q1 is a full charge and Q2 is a partial charge, F is
comparatively large.
• F increases as Q increases and as d decreases:
– the larger the charge and smaller the ion, the larger the
F =
Trang 8Intermolecular Forces
Trang 9Intermolecular Forces
Dipole-Dipole Forces (l ực lưỡng cực-lưỡng cực)
• Interaction between a dipole (e.g water) and a
dipole (e.g water)
• Dipole-dipole forces exist between neutral polar molecules (giữa các phân tử phân cực trunghoà).
• Polar molecules need to be close together.
• Weaker than ion-dipole forces :
2 2
1 Q
Q k
F =
Trang 10• If two molecules have about the
same mass and size, then dipole-dipole forces increase with increasing polarity.
Trang 11Intermolecular Forces
London Dispersion Forces
• Weakest of all intermolecular forces.
• It is possible for two adjacent (kề nhau) neutral
molecules to affect each other.
• The nucleus of one molecule (or atom) attracts the
electrons of the adjacent molecule (or atom).
• For an instant, the electron clouds become
distorted.
• In that instant a dipole is formed (called an
instantaneous dipole-lưỡng cực tạm thời) .
Trang 12Intermolecular Forces
London Dispersion Forces
Trang 13Intermolecular Forces
London Dispersion Forces
• One instantaneous dipole can induce (tác động)
another instantaneous dipole in an adjacent
molecule (or atom).
• The forces between instantaneous dipoles are
called London dispersion forces.
• Polarizability is the ease with which an electron
cloud can be deformed.
• The larger the molecule (the greater the number
of electrons) the more polarizable
Trang 14Intermolecular Forces
London Dispersion Forces
Trang 15Intermolecular Forces
London Dispersion Forces
• London dispersion forces increase as molecular weight increases.
• London dispersion forces exist between all
molecules.
• London dispersion forces depend on the shape
of the molecule.
• The greater the surface area available for
contact, the greater the dispersion forces.
• London dispersion forces between spherical
Trang 16Intermolecular Forces
• Special case of dipole-dipole forces
• By experiments: boiling points of compounds
with H-F, H-O, and H-N bonds are abnormally high.
• Intermolecular forces are abnormally strong.
• H-bonding requires H bonded to an
electronegative element (most important for
Trang 17Intermolecular Forces
Hydrogen Bonding
Trang 18Intermolecular Forces
Hydrogen Bonding
Hydrogen bonds are responsible for:
– Ice Floating
• Solids are usually more closely packed than liquids;
• therefore, solids are more dense than liquids.
• Ice is ordered with an open structure to optimize H-bonding.
• Therefore, ice is less dense than water.
• In water the H-O bond length is 1.0 Å.
• The O…H hydrogen bond length is 1.8 Å.
• Ice has waters arranged in an open, regular hexagon.
• Each δ+ H points towards a lone pair on O.
• Ice floats, so it forms an insulating layer on top of lakes, rivers,
etc Therefore, aquatic life can survive in winter.
Trang 19Intermolecular Forces
Hydrogen Bonding
• Hydrogen bonds are responsible for:
– Protein Structure
• Protein folding is a consequence of H-bonding.
• DNA Transport of Genetic Information
Trang 20Intermolecular Forces
Comparing Intermolecular Forces
Trang 21Some Properties of Liquids
Viscosity (độ nhớt)
• Viscosity is the resistance of a liquid to flow.
• A liquid flows by sliding molecules over each
other.
• The stronger the intermolecular forces, the
higher the viscosity.
Surface Tension (sức căng bề mặt)
• Bulk molecules (those in the liquid) are equally
attracted to their neighbors.
Trang 22Some Properties of Liquids
Surface Tension
Trang 23Some Properties of Liquids
Surface Tension
• Surface molecules are only attracted inwards towards the bulk molecules.
– Therefore, surface molecules are packed more
closely than bulk molecules.
• Surface tension is the amount of energy
required to increase the surface area of a liquid.
• Cohesive forces (lực cố kết) bind molecules to each other.
• Adhesive forces (lực kết dính ) bind molecules to
Trang 24Some Properties of Liquids
Surface Tension
Trang 25Some Properties of Liquids
Surface Tension
• Meniscus is the shape of the liquid surface
– If adhesive forces are greater than cohesive forces, the liquid surface is attracted to its container more than the bulk molecules Therefore, the meniscus is U-shaped (e.g water in glass).
– If cohesive forces are greater than adhesive forces, the
meniscus is curved downwards
• Capillary Action: When a narrow glass tube is
placed in water, the meniscus pulls the water up the tube.
Trang 26Phase Changes
• Surface molecules are only attracted inwards
towards the bulk molecules.
• Sublimation: solid → gas.
• Vaporization: liquid → gas.
• Melting or fusion: solid → liquid.
• Deposition: gas → solid.
• Condensation: gas → liquid.
• Freezing: liquid → solid.
Energy Changes Accompanying Phase Changes
• Energy change of the system for the above
processes are:
Trang 27Phase Changes
Energy Changes Accompanying Phase
Changes
– Sublimation: ∆Hsub > 0 (endothermic)
– Vaporization: ∆Hvap > 0 (endothermic).
– Melting or Fusion: ∆Hfus > 0 (endothermic).
– Deposition: ∆Hdep < 0 (exothermic)
– Condensation: ∆Hcon < 0 (exothermic).
– Freezing: ∆Hfre < 0 (exothermic).
• Generally heat of fusion (enthalpy of fusion) is
Trang 28Phase Changes
Energy Changes Accompanying Phase Changes
• All phase changes are possible under the right
conditions (e.g water sublimes when snow
disappears without forming puddles).
Trang 29Phase Changes
Energy Changes Accompanying Phase Changes
Trang 30Phase Changes
Heating Curves / Cooling curves
• Plot of temperature change versus heat added is
a heating curve.
• During a phase change, adding heat causes no
temperature change.
– These points are used to calculate ∆Hfus and ∆Hvap
• Supercooling : When a liquid is cooled below its melting point and it still remains a liquid.
• Achieved by keeping the temperature low and
increasing kinetic energy to break
intermolecular forces.
Trang 31Phase Changes
Heating Curves
Trang 32Phase Changes
Critical Temperature and Pressure
• Gases liquefied by increasing pressure at some
temperature.
temperature for liquefaction of a gas using pressure.
for liquefaction.
Trang 33Vapor Pressure
Explaining Vapor Pressure on the Molecular
Level
• Some of the molecules on the surface of a liquid have
enough energy to escape the attraction of the bulk
liquid.
• These molecules move into the gas phase.
• As the number of molecules in the gas phase increases,
some of the gas phase molecules strike the surface and return to the liquid.
• After some time the pressure of the gas will be
Trang 34Vapor Pressure
Explaining Vapor Pressure on the Molecular Level
• Dynamic Equilibrium: the point
when as many molecules escape the surface as strike the surface.
• Vapor pressure is the pressure
exerted when the liquid and vapor are in dynamic
equilibrium.
Trang 35Vapor Pressure
Volatility, Vapor Pressure, and Temperature
• If equilibrium is never established then the liquid
evaporates.
• Volatile substances evaporate rapidly.
• The higher the temperature, the higher the average
kinetic energy, the faster the liquid evaporates.
Trang 36Vapor Pressure
Volatility, Vapor Pressure, and Temperature
Trang 37Vapor Pressure
Vapor Pressure and Boiling Point
• Liquids boil when the external pressure equals the
reducing the cooking time required.
Trang 38Phase Diagrams
• Phase diagram: plot of pressure vs Temperature
summarizing all equilibria between phases.
• Given a temperature and pressure, phase diagrams
tell us which phase will exist.
• Features of a phase diagram:
– Triple point: temperature and pressure at which all three
phases are in equilibrium
– Vapor-pressure curve: generally as pressure increases,
Trang 39Phase Diagrams
• Any temperature and pressure combination not on a
curve represents a single phase.
Trang 40– Triple point occurs at 0.0098°C and 4.58 mmHg.
– Normal melting (freezing) point is 0°C.
– Normal boiling point is 100°C.
– Critical point is 374°C and 218 atm.
• Carbon Dioxide:
– Triple point occurs at -56.4°C and 5.11 atm.
– Normal sublimation point is -78.5°C (At 1 atm CO 2 sublimes
it does not melt.)
Trang 41Phase Diagrams
The Phase Diagrams of H2O and CO2
Trang 42Structures of Solids
Unit Cells
• Crystalline solid: well-ordered, definite arrangements
of molecules, atoms or ions
• Crystals have an ordered, repeated structure.
• The smallest repeating unit in a crystal is a unit cell.
• Unit cell is the smallest unit with all the symmetry of
the entire crystal.
• Three-dimensional stacking of unit cells is the crystal
lattice.
Trang 43Structures of Solids
Unit Cells
Trang 44Structures of Solids
Unit Cells
• Three common types of unit cell.
– Primitive cubic, atoms at the corners of a simple cube,
• each atom shared by 8 unit cells;
– Body-centered cubic (bcc), atoms at the corners of a cube plus one in the center of the body of the cube,
• corner atoms shared by 8 unit cells, center atom completely enclosed in one unit cell;
– Face-centered cubic (fcc), atoms at the corners of a cube plus one atom in the center of each face of the cube,
• corner atoms shared by 8 unit cells, face atoms shared by 2 unit
cells.
Trang 45Structures of Solids
Unit Cells
Trang 46Structures of Solids
Crystal Structure of Sodium Chloride
• Face-centered cubic lattice.
• Two equivalent ways of defining unit cell:
– Cl - (larger) ions at the corners of the cell, or
– Na + (smaller) ions at the corners of the cell.
• The cation to anion ratio in a unit cell is the same for
the crystal In NaCl each unit cell contains same number of Na+ and Cl- ions.
• Note the unit cell for CaCl2 needs twice as many Cl
-ions as Ca2+ ions.
Trang 47Structures of Solids
Crystal Structure of Sodium Chloride
Trang 48Structures of Solids
Close Packing of Spheres
• Solids have maximum intermolecular forces.
• Molecules can be modeled by spheres.
• Atoms and ions are spheres.
• Molecular crystals are formed by close packing of the
molecules.
• We rationalize maximum intermolecular force in a
crystal by the close packing of spheres.
• When spheres are packed as closely as possible, there
are small spaces between adjacent spheres.
• The spaces are called interstitial holes.
Trang 49Structures of Solids
Close Packing of Spheres
Trang 50Structures of Solids
Close Packing of Spheres
• A crystal is built up by placing close packed layers of
spheres on top of each other.
• There is only one place for the second layer of spheres.
• There are two choices for the third layer of spheres:
– Third layer eclipses the first (ABAB arrangement) This is
called hexagonal close packing (hcp);
– Third layer is in a different position relative to the first
(ABCABC arrangement) This is called cubic close packing (ccp).
Trang 51Structures of Solids
Close Packing of Spheres
Trang 52Structures of Solids
Close Packing of Spheres
• Each sphere is surrounded by 12 other spheres (6 in
one plane, 3 above and 3 below).
• Coordination number: the number of spheres directly
surrounding a central sphere.
• Hexagonal and cubic close packing are different from
the cubic unit cells.
• If unequally sized spheres are used, the smaller
spheres are placed in the interstitial holes.
Trang 53Structures of Solids
X-Ray Diffraction
• When waves are passed through a narrow slit
they are diffracted.
• When waves are passed through a diffraction
grating (many narrow slits in parallel) they
interact to form a diffraction pattern (areas of
light and dark bands).
• Efficient diffraction occurs when the wavelength
of light is close to the size of the slits.
• The spacing between layers in a crystal is 2 - 20
Å, which is the wavelength range for X-rays.
Trang 54Structures of Solids
X-Ray Diffraction
Trang 55Structures of Solids
X-Ray Diffraction
• X-ray diffraction (X-ray crystallography):
– X-rays are passed through the crystal and are
detected on a photographic plate.
– The photographic plate has one bright spot at the
center (incident beam) as well as a diffraction pattern.
– Each close packing arrangement produces a different
diffraction pattern.
– Knowing the diffraction pattern, we can calculate the
positions of the atoms required to produce that
pattern.
– We calculate the crystal structure based on a
Trang 56Bonding in Solids
– Molecular (formed from molecules) - usually soft
with low melting points and poor conductivity.
with very high melting points and poor conductivity.
points and poor conductivity.
high melting points, good conductivity, malleable
and ductile.
Trang 57Bonding in Solids
Trang 58• Room temperature gases and liquids usually
form molecular solids at low temperature.
• Efficient packing of molecules is important
(since they are not regular spheres).
Trang 59Bonding in Solids
Covalent Network Solids
• Intermolecular forces: dipole-dipole, London dispersion and H-bonds.
• Atoms held together in large networks.
• Examples: diamond, graphite, quartz (SiO2),
silicon carbide (SiC), and boron nitride (BN).
• In diamond:
– each C atom has a coordination number of 4;
– each C atom is tetrahedral;
– there is a three-dimensional array of atoms.
Trang 60Bonding in Solids
Covalent Network Solids