Solid Particles are packed very closely Cannot be compressed Fixed in volume Held together by a very strong force of attraction (Eg. Electrostatic forces, intermolecular forces) 2 types: crystalline solid n amorphous solid Types of Solids Crystalline Amorphous Particles Regular repeating 3D geometric Randomly arranged and not in arrangement structure order Shapes Well-defined edges and faces Irregular or curved surfaces Melting point Sharp melting and boiling points Melt over a wide range of temperature Examples Salts (NaCl), quartz (SiO2), Rubber, plastics, glove metals, diamonds Ionic solids Applies to ionic cmpd Giant ionic structure Alternating positive (cations) and negative (anions) Held together by strong electrostatic forces (btw cations & anions) 1. NaCl o Na+ ion (cation) donate 1 ion to anions o Cl- (anion) receive 1 extra ions, electron cloud become bigger compared to the metal cation o Unit cell: Face centered cubic (FCC) Each Na+ ions surrounded by 6 Cl- ions Each Cl- ions surrounded by 6 Na+ ions o Coordination number = 6 (both Na+ ions & Cl- ions) 2. MgO o Mg2+ (cation); O2- (anion) o Unit cell: face centered cubic (FCC) Physical Properties : *Anion (bigger size) : occupy the corner & face center *Cation (smaller size) : fill the voids o Hard Strong electrostatic forces Surface can’t be scratched easily o Brittle When a strong force is applied, layers of ion will be displacing, ions of the same charge will become adjacent. Thus, create a repulsion that cause crystal to shatter and cracks o Solubility Soluble in water but not in organic solvent Polar water molecule attracted to ions in NaCl Na+ (cations) attracted to partially negative region (𝛿 − ) of water molecule (O) Cl- (anions) attracted to partially positive region (𝛿 + ) of water molecule (H) Attraction between polar water molecules and ions in NaCl pull the ions away from the crystal lattice, hence collapsing crystal lattice in NaCl o o High melting points and boiling points Due to the strong electrostatic force of attraction between the cations and anions Requires a lot of heat energy to overcome them MgO has higher boiling point compare to NaCl Factors affecting: Charge of the ions - Higher charge, stronger electrostatic attractions, stronger bonds - Eg. MgO (2+/2-) attract each other more strongly than NaCl (1+/1-) Size of the ions - Smaller ions are arranged closer together, stronger electrostatic attractions - Eg. NaCl melts at 801°C and Rubidium iodine melts at 674°C (NaCl has smaller size compared to RbI) Electrical conductivity Does not conduct electricity in solid form Ions are strongly held by electrostatic force and Ions in a fixed position in crystal lattice. Ions are not free to moves Conduct electricity in aqueous or molten form Ions are free to move. Electrolytes are one of the examples. Ions will be carrying electrical current Simple molecular / covalent solids Btw the molecules : IMF (VdW forces) Simple covalent mlcs In the molecules : Covalent bond Eg. CO2, I2, P4, S8 Held together by weak intermolecular forces (IMF) btw the molecule (Van der Waals attraction / Hydrogen bonding) 1. Iodine (I2) o Unit cell: Face center cubic (FCC) o Molecules are closely packed but they are still separate molecule o Forces: weak intermolecular forces – Van der Waals forces 2. Ice o Oxygen atom of each water molecule forms hydrogen bonds with two hydrogen atoms of nearby water molecule -> 3D tetrahedral arrangement o One water molecule able to form 4 hydrogen bonds o Extensive hydrogen bonding very open structure molecule further apart from each other compared to liquid form less dense in water Physical properties: o Low melting point Weak intermolecular forces Tend to be gases, liquid at room temperature Larger molecules increase more surface area between molecules more IMF attractions more energy is needed to break down the bond increase the melting n boiling point Presence of hydrogen bonding, melting n boiling point increase too o Sparingly soluble in water Soluble in organic solvents o Non-conductors of heat or electricity No free ions / don’t have free delocalised e when they are in water Giant covalent solid structure Non-metallic atoms Joined by extended network of covalent bonds (intramolecular forces) No discrete molecule is present Higher melting and boiling points than simple molecular solids Eg. Allotropes of carbon: Diamond or graphite / quartz (silicon (IV) oxide) [ Allotropes= carbon which can exist more than 1 form by having difference in arrangement of atoms ] 1. Diamond o Sp3 hybridization and 109.5° bond angle o Coordination number= 4 (4 single covalent bonds) o Each carbon is bonded to 4 neighboring carbon o Extended network of covalent bond o Physical properties Very high melting and boiling point Due to the very strong carbon-carbon covalent bonds must be broken throughout the structure before melting occurs (Extended network of covalent bond) Very hard The atoms are held by strong covalent bond & hard to break Doesn’t conduct electricity All the electrons are held tightly between the atoms, and aren’t free to move Insoluble in water and organic solvents Attractions between solvent molecule and carbon atoms will never be strong enough to overcome the strong covalent bonds in diamond 2. Graphite o 2d layers of hexagonal rings o Planar structure and sp2 hybridization and 120° bond angle o o Unhybridized p orbital – 1 free electron Can be delocalized throughout the lattice account for the electrical conductivity Coordination number = 3 (can form 3 single covalent bonds) Physical properties High melting and boiling points Due to strong covalent bonds (between carbons) in each layer. High energy is needed to overcome this strong bond Soft and slippery Easily scratched. Layers of graphite can slide over each when a force is applied due to weak intermolecular force (between layers) pencil lead Good electrical conductors Due to the presence of pi electrons that are freely delocalised through the entire sheet. / The delocalised electrons can move along the layer (when voltage is applied) Insoluble in water and organic solvents Attractions between solvent molecule and carbon atoms will never be strong enough to overcome the strong covalent bonds in graphite Diamond Transparent (able to see through) High density Non-electrical conductor no delocalize electron Graphite Black and opaque (can’t see through) Lower density than diamond between the sheets has wasted relatively large amount of space Electrical conductor delocalize electron in the π bond 3. Silicon dioxide o Tetrahedral arrangement Each silicon atom is bonded to 4 oxygen atoms Each oxygen atom is bonded to 2 silicon atoms o Has strong network of covalent bond o Sp3 hybridization and 109.5° bond angle o Coordination number= 4 o Physical properties Very high melting and boiling point Due to the very strong carbon-carbon covalent bonds must be broken throughout the structure before melting occurs Very hard Due to need to break very strong covalent bonds operating in 3D Doesn’t conduct electricity All the electrons are held tightly between the atoms, and aren’t free to move Insoluble in water and organic solvents Attractions between solvent molecule and silicon atoms nor oxygen atoms will never stronger to overcome the strong covalent bonds in silicon dioxide Metallic solid Bonding : Metallic bond [ Strong electrostatic attraction btw metallic cations (+ve) & ‘sea’ of electrons (-ve) ) 1. Copper o Unit cell: Face-centered cubic (FCC) o Coordination number = 12 o Physical properties Hard, high melting and boiling points Strong metallic bond Size cations bigger the size of atoms, larger distance between nucleus and valence electrons, decrease in strength of metallic bond No. of valence electrons increase in no. of valence electron, increase in strength of metallic bond Good electrical conductors (Conduct electricity in both solid & molten state) Due to delocalised sea of electron that are free to move Good thermal/heat conductors Heat energy picked up by electrons (additional kinetic energy) move faster Good strength / Not brittle Does not shatter when force is applied (not brittle) The metallic bonds do not break as electrons are free to move High flexibility Malleability (deformed under compression) Eg. Flatten in a sheet Ductility (deformed under tension) Eg. Pulled out into wires The presence of layers in crystal lattice that can slide over on another Metallic bonds are non-directional : electrons can take up new positions & reform after deformation When a force is applied, one plane of metal ions will be slides over another. The delocalized electrons take up new position and the metallic bond can be maintained. (Due to non-directional) Gas Particles far apart and collide between each other Can be compressed small particles + far apart Mix evenly confined into the same container [Effusion]; Manage to escape through tiny hole of container [Diffusion] Exert pressure uniformly on all sides of a container Relatively low densities Force = Pressure 1 atm= 760 mmHg = 760 torr = 101325 Pa = 101325 Nm-2 Area [STP] 𝐺𝑖𝑣𝑒𝑛 𝑢𝑛𝑖𝑡 × 𝐷𝑒𝑠𝑖𝑟𝑒𝑑 𝑢𝑛𝑖𝑡 = 𝐷𝑒𝑠𝑖𝑟𝑒𝑑 𝑢𝑛𝑖𝑡 𝐺𝑖𝑣𝑒𝑛 𝑢𝑛𝑖𝑡 Gas Law Boyle’s Law 1 [ 𝑃𝑉 = 𝑘] 𝑃∝ 𝑉 T (fixed) Charles’ Law 𝑉 𝑉 ∝ 𝑇 [ = 𝑘] 𝑇 P (fixed) Gay-Lussac’s Law 𝑃 𝑃 ∝ 𝑇 [ = 𝑘] 𝑇 V (fixed) Avogadro’s Law 𝑉 𝑉 ∝ 𝑛 [ = 𝑘] 𝑛 T & P (fixed) [ 𝑃 ↑, 𝑉 ↓ ] [ 𝑇 ↑, 𝑉 ↑ ] [ 𝑇 ↑, 𝑃 ↑ ] [ 𝑛𝑜. 𝑜𝑓 𝑚𝑜𝑙𝑒𝑠 ↑, 𝑉 ↑ ] 𝑃1 𝑉1 = 𝑃2 𝑉2 𝑉1 𝑉2 = 𝑇1 𝑇2 𝑃1 𝑃2 = 𝑇1 𝑇2 𝑉1 𝑉2 = 𝑛1 𝑛2 n= No. of moles Combine Gas Law 𝑃1 𝑉1 𝑃2 𝑉2 = 𝑇1 𝑇2 Molar Volume STP: 1 mol of gas is 22.4L Room temperature : 1 mole of gas is 24L Volume (L/dm3) = mol × molar volume *Temperature must be in kelvin (K) 1°C = 273K **STP = 1atm and 0°C Charles’ Law Gay-Lussac’s Law Ideal Gas Law 𝑃𝑉 = 𝑛𝑅𝑇 1. Molar mass o 𝑀= 𝑚𝑅𝑇 𝑃𝑉 2. Density o 𝜌= 𝑀𝑃 𝑅𝑇 P Pressure (atm) V Volume (L) n no. of mole (mole) R Universal gas content (0.08206 atm.L/mol.K) T Temperature (K) g Mass (g) M Molar mass (g mol-1) Dalton’s Law of partial pressure The total pressure of a mixture of gases in one container is the sum of the pressure of individual 𝑃𝑡𝑜𝑡𝑎𝑙 = 𝑃1 + 𝑃2 + 𝑃3 … o 𝑃𝑇 = 𝑃𝐴 + 𝑃𝐵 𝑛 𝑅𝑇 𝑛 𝑅𝑇 = 𝐴𝑉 + 𝐵𝑉 𝑅𝑇 = (𝑛𝐴 + 𝑛𝐵 ) 𝑉 𝑅𝑇 = (∑𝑛) 𝑉 𝑛𝐴 → 𝑛𝑜. 𝑜𝑓 𝑚𝑜𝑙𝑒𝑠 𝑜𝑓 𝑔𝑎𝑠 𝐴 𝑛𝐵 → 𝑛𝑜. 𝑜𝑓 𝑚𝑜𝑙𝑒𝑠 𝑜𝑓 𝑔𝑎𝑠 𝐵 If total pressure is given, then use the formula 𝑛𝐴 +𝑛 𝐴 𝐵 (𝑛𝑇 ) 𝑛𝐵 𝑛𝑇 𝑋𝐴 → 𝑛 𝑋𝐵 → o 𝑃𝐴 = 𝑋𝐴 𝑃𝑇 ; 𝑃𝐵 = 𝑋𝐵 𝑃𝑇 Deviation from Ideal Gas Behaviour Ideal gas : A gas which obeys the gas laws and gas eq (PV = nRT) strictly at all conditions of temperature and pressure. Real gases : The gases that obeys the gas laws fairly well if the pressure is low OR the temperature is high. *Deviation from ideal gas behaviour are observed particularly : - At HIGH pressure - At LOW temperature 𝑃𝑉 𝑉 Compressibility factor, Z [𝑍 = 𝑛𝑅𝑇 = 𝑉 𝑟𝑒𝑎𝑙 ] 𝑖𝑑𝑒𝑎𝑙 For ideal gas, 𝑃𝑉 = 𝑛𝑅𝑇 ∴ 𝑍 = 1 For real gas, 𝑃𝑉 ≠ 𝑛𝑅𝑇 ∴ 𝑍 ≠ 1 o Therefore Z can be < 1 OR > 1 : o When Z < 1, it is a negative deviation. It shows that the gas is more compressible than expected from ideal behaviour. (Eg: CH4, CO2, etc) o When Z > 1, it is a positive deviation. It shows that the gas is less compressible than expected from ideal behaviour. Causes of Deviation from ideal behaviour Due to 2 wrong assumptions of Kinetic Theory of Gases : 1. When compared to the total volume of the gas, the volume occupied by gas molecules is negligible 2. The force of attraction (IMF) btw gas molecules are negligible [The assumptions ONLY true at LOW pressure & HIGH temperature - as the distance btw the molecules is large] Ideal Gas Assumptions fits Kinetic Theory of Gases o Are in random motion in straight line o Have perfect elastic collision. No loss in kinetic energy during Collision. o The average kinetic energy is directly proportional to Kelvin temperature of the gas o The volume occupied by the molecule themselves is entirely negligible relative to the volume of the container. o Negligible intermolecular forces between molecules. Obeys ideal gas laws [ 𝑃𝑉 = 𝑛𝑅𝑇 ] False! ! Compressibility factor, Z = 1 (if n=1) – A straight line Gas will behave ideally when : Low pressure Volume of gas particles is negligible and relatively small compared to the volume of container. IMF negligible due to bigger volume of the container High temperature molecules higher kinetic energy and moving at high speed. They can easily overcome the IMF attraction between molecule Real Gas Only obeys ideal gas laws where the pressure is low, and temperature is high Do not always the kinetic theory o The volume occupied by the molecule themselves is entirely may not negligible relative to the volume of the container. When the pressure is high, and temperature is low molecules being incompressible volume of molecules is no more negligible as compared to the total volume of the gas o The force of attraction btw gas molecules are negligible TRUE when at low pressure & high temperature When the pressure is high, and temperature is low total volume of gas is small forces of attraction become can’t negligible High pressure Low temperature -More molecules / High density (small -kinetic energy relatively smaller volume) molecules move in low speed -Closer from each other Increase in IMF -IMF increase less collision to the wall (no more negligible) lower pressure is observed Compressibility factor, Z ≠ 1 o Positive deviation, Z > 1 [Due to volume] Above the line of ideal gas (gas is less compressible expected than from ideal behavior) o Negative deviation, Z < 1 [Due to IMF] Below the line of ideal gas (gas is more compressible than expected from ideal behavior) Higher temperature, gas behaves more ideally (less deviation)