States of Matter – Comprehensive Notes (for NEET/JEE)
Matter exists in different physical forms, or “states,” depending on the conditions of temperature and pressure. Understanding these states and the transitions between them is fundamental to comprehending the physical behavior of substances. This chapter is exceptionally crucial for NEET and JEE Main, particularly the Gas Laws, deviations from ideal behavior, and properties of liquids.
1. Introduction to States of Matter
- Matter: Anything that possesses mass and occupies space. It is composed of particles (atoms, molecules, or ions).
- States of Matter: The physical state of a substance is primarily determined by the delicate balance between two opposing forces:
- Intermolecular forces of attraction: These forces tend to pull and hold particles closer together.
- Thermal energy of the particles: This energy (related to kinetic energy) tends to keep particles moving and far apart.
- Solid State: Intermolecular forces are overwhelmingly dominant compared to thermal energy. Particles are tightly packed in fixed positions, vibrating about their mean positions.
- Liquid State: Intermolecular forces are comparable to thermal energy. Particles are closely packed but possess enough thermal energy to overcome fixed positions and slide past each other.
- Gaseous State: Thermal energy is much greater than intermolecular forces. Particles are far apart, moving rapidly and randomly.
- Phase Transitions: Processes where matter changes from one physical state to another. These transitions are always accompanied by characteristic energy changes (either absorption or release of heat) at constant temperature.
2. The Gaseous State
Gases exhibit unique macroscopic properties due to the large average distances between their constituent particles and the negligible intermolecular forces between them under normal conditions.
2.1. Characteristics of Gases
- Indefinite Shape and Volume: Gases completely fill the container they occupy, taking its shape and volume.
- High Compressibility: Due to large intermolecular spaces, gases can be compressed significantly.
- Low Density: Compared to solids and liquids, gases have very low densities because particles are widely spaced.
- Constant, Random Motion: Gas particles are in continuous, chaotic motion, colliding with each other and the container walls.
- Uniform Pressure Exertion: Gases exert pressure equally in all directions on the walls of their container.
- High Diffusibility: Gases readily intermix and spread uniformly throughout another gas or a vacuum.
2.2. Gas Laws (Ideal Gas Behavior)
These empirical laws describe the quantitative relationships between pressure (P), volume (V), temperature (T, always in Kelvin), and number of moles (n) for an ideal gas. An ideal gas is a hypothetical gas that strictly obeys these laws under all conditions.
- 1. Boyle’s Law (Pressure-Volume Relationship, at constant n, T):
- Statement: At constant temperature and a fixed amount of gas, the pressure of the gas is inversely proportional to its volume.
- Formula: P∝1/V or PV=constant or P1V1=P2V2
- Graphical Representation:
- P vs 1/V plot: A straight line passing through the origin.
- P vs V plot: A hyperbola (also called an isotherm). Each curve on a P-V graph represents a different constant temperature.
- Log P vs Log V plot: A straight line with a negative slope (-1).
- 2. Charles’s Law (Volume-Temperature Relationship, at constant n, P):
- Statement: At constant pressure and a fixed amount of gas, the volume of the gas is directly proportional to its absolute temperature (Kelvin).
- Formula: V∝T or V/T=constant or V1/T1=V2/T2
- Graphical Representation:
- V vs T plot: A straight line passing through the origin (if temperature is in Kelvin). This is called an isobar.
- If V vs T (∘C) is plotted, the line extrapolates to -273.15$^\circ C$ (0 K) at zero volume, defining absolute zero.
- 3. Gay-Lussac’s Law (Pressure-Temperature Relationship, at constant n, V):
- Statement: At constant volume and a fixed amount of gas, the pressure of the gas is directly proportional to its absolute temperature (Kelvin).
- Formula: P∝T or P/T=constant or P1/T1=P2/T2
- Graphical Representation:
- P vs T plot: A straight line passing through the origin (if temperature is in Kelvin). This is called an isochore.
- 4. Avogadro’s Law (Volume-Mole Relationship, at constant P, T):
- Statement: Equal volumes of all gases contain an equal number of moles (or molecules) under the same conditions of temperature and pressure.
- Formula: V∝n or V/n=constant
- Consequence: At STP (Standard Temperature and Pressure: 0°C or 273.15 K, 1 atm or 101.325 kPa), 1 mole of any ideal gas occupies 22.4 liters (molar volume). At SATP (Standard Ambient Temperature and Pressure: 25°C or 298.15 K, 1 bar or 100 kPa), 1 mole of any ideal gas occupies 22.7 liters.
2.3. Combined Gas Law and Ideal Gas Equation
- Combined Gas Law: This law combines Boyle’s, Charles’, and Gay-Lussac’s laws. It is useful when the amount of gas is constant but pressure, volume, and temperature change.
- Formula: (P1V1)/T1=(P2V2)/T2
- Formula: (P1V1)/T1=(P2V2)/T2
- Ideal Gas Equation: This equation is a single mathematical expression that describes the relationship between all four variables (P, V, n, T) for an ideal gas. It combines all four gas laws.
- Formula: PV=nRT
- R = Universal Gas Constant: Its value depends on the units used for P, V, and T.
- R=0.0821 L atm mol−1 K−1
- R=8.314 J mol−1 K−1 (SI unit)
- R=8.314×107 erg mol−1 K−1
- R=1.987≈2 cal mol−1 K−1
- R=0.0821 L atm mol−1 K−1
- R = Universal Gas Constant: Its value depends on the units used for P, V, and T.
- Density of an Ideal Gas: The ideal gas equation can be rearranged to relate density (d) to other parameters.
- Since n=mass(m)/Molar mass(M), substitute into PV=nRT: PV=(m/M)RT
- Rearranging to solve for density (d=m/V): PM=(m/V)RT⇒PM=dRT d=PM/RT
- Implication: Gas density is directly proportional to pressure and molar mass, and inversely proportional to temperature. This is important for relative densities and determining molar masses of unknown gases.
- Since n=mass(m)/Molar mass(M), substitute into PV=nRT: PV=(m/M)RT
- Formula: PV=nRT
2.4. Dalton’s Law of Partial Pressures
- Statement: For a mixture of non-reacting gases confined in a container, the total pressure exerted by the mixture is equal to the sum of the partial pressures that each individual gas would exert if it alone occupied the entire volume of the container at the same temperature.
- Formula: Ptotal=P1+P2+P3+…+Pn (where P1,P2, etc. are partial pressures).
- Partial Pressure: The pressure exerted by an individual gas in a mixture.
- Relationship with Mole Fraction: The partial pressure of a gas is directly proportional to its mole fraction in the mixture.
- Pi=Xi×Ptotal
- Where Pi is the partial pressure of gas ‘i’, Xi is the mole fraction of gas ‘i’ (moles of gas ‘i’ / total moles of gases), and Ptotal is the total pressure of the gas mixture.
- Pi=Xi×Ptotal
- Application: Collection of Gas Over Water (Wet Gas): When a gas is collected over water, it is saturated with water vapor. The total pressure measured is the sum of the pressure of the dry gas and the aqueous tension (vapor pressure of water at that specific temperature).
- Pdry gas=Ptotal−Paqueous tension
- Pdry gas=Ptotal−Paqueous tension
2.5. Graham’s Law of Diffusion/Effusion
- Diffusion: The spontaneous intermixing of gas molecules due to their random motion, leading to a uniform distribution throughout the available volume.
- Effusion: The process by which a gas escapes from a container through a very small opening (pinhole) into a vacuum or a region of lower pressure.
- Statement: At constant temperature and pressure, the rate of diffusion or effusion of a gas is inversely proportional to the square root of its molar mass (or density).
- Formula: r∝1/M or r∝1/d
- For two gases, 1 and 2:
r1/r2=M2/M1=d2/d1 - Rate (r) can be expressed as:
- Volume diffused / time
- Moles diffused / time
- Distance diffused / time
- Key Consideration: For effusion, the hole must be very small so that gas particles do not collide near the hole.
- Formula: r∝1/M or r∝1/d
2.6. Kinetic Molecular Theory of Gases (KMT)
KMT provides a theoretical foundation for the observed macroscopic behavior of ideal gases. It is based on a set of fundamental postulates:
- Postulates:
- Tiny Particles: Gases consist of a very large number of identical, tiny particles (atoms or molecules) that are very far apart from each other. The actual volume occupied by the gas molecules themselves is negligible compared to the total volume of the container.
- Constant, Random Motion: Gas particles are in a state of continuous, rapid, and random motion in all possible directions.
- Negligible Intermolecular Forces: There are no significant attractive or repulsive forces between gas molecules. They move independently of each other.
- Elastic Collisions: Collisions between gas molecules themselves, and between gas molecules and the walls of the container, are perfectly elastic. This means that there is no net loss of kinetic energy during collisions (though kinetic energy may be transferred between molecules).
- Average Kinetic Energy and Temperature: The average kinetic energy of the gas molecules is directly proportional to the absolute temperature (in Kelvin).
KEavg=(3/2)kT Where k is the Boltzmann constant (k=R/NA, where R is the gas constant and NA is Avogadro’s number). This means at a given temperature, all ideal gases (regardless of their nature) have the same average kinetic energy.
- Speeds of Gas Molecules: Due to constant random motion, gas molecules have a range of speeds.
- Root Mean Square (RMS) Speed (urms): The square root of the mean of the squares of the speeds of the individual molecules. It reflects the average kinetic energy.
urms=3RT/M - Average Speed (uavg): The arithmetic mean of the speeds of all molecules.
uavg=8RT/πM - Most Probable Speed (ump): The speed possessed by the maximum fraction of molecules at a given temperature.
ump=2RT/M - Order of Speeds: ump<uavg<urms (approximately in the ratio 1 : 1.128 : 1.224)
- Root Mean Square (RMS) Speed (urms): The square root of the mean of the squares of the speeds of the individual molecules. It reflects the average kinetic energy.
2.7. Real Gases (Deviations from Ideal Behavior)
- Ideal Gas: A hypothetical gas that perfectly adheres to the ideal gas equation (PV=nRT) and the postulates of KMT under all conditions.
- Real Gases: All gases found in nature are real gases. They deviate from ideal behavior, especially under conditions of high pressure and low temperature.
- Reasons for Deviation (Failure of KMT Postulates):
- Finite Volume of Molecules (Volume Correction): The KMT assumes gas molecules have negligible volume. However, at high pressures, the volume occupied by the gas molecules themselves becomes significant compared to the total volume of the container. The actual volume available for the motion of molecules is effectively less than the measured volume of the container.
- Presence of Intermolecular Forces (Pressure Correction): The KMT assumes no attractive or repulsive forces between molecules. However, at low temperatures, molecules move more slowly, allowing intermolecular forces of attraction to become significant. These attractive forces pull molecules towards each other, reducing the frequency and force of collisions with the container walls. This leads to a lower observed pressure than would be expected for an ideal gas.
- Compressibility Factor (Z): A quantitative measure of the deviation of real gases from ideal behavior.
- Formula: Z=PV/nRT
- For an ideal gas, Z=1 at all temperatures and pressures.
- For Real Gases:
- When Z < 1 (Negative Deviation): This occurs when attractive forces between molecules are dominant. The gas is more compressible than an ideal gas. (Observed at relatively low pressures and moderate temperatures for most gases like CO2, CH4).
- When Z > 1 (Positive Deviation): This occurs when repulsive forces become dominant, primarily due to the finite volume occupied by the molecules themselves. The gas is less compressible than an ideal gas. (Observed at very high pressures for all gases, or for very small molecules like H2 and He at almost all pressures, due to their weak attractive forces).
- At very low pressures: Real gases tend to behave ideally (Z approaches 1) because molecules are far apart and intermolecular forces are negligible.
- Formula: Z=PV/nRT
- Van der Waals Equation (for Real Gases): J.D. van der Waals modified the ideal gas equation to account for the two main defects of KMT.
- Equation: (P+a(n2/V2))(V−nb)=nRT
- ‘a’ (Pressure Correction Term / Attraction Term): Corrects for the intermolecular attractive forces.
- Its value depends on the nature of the gas.
- A larger ‘a’ value indicates stronger attractive forces between gas molecules.
- Units of ‘a’: atm L2 mol-2 or Pa m6 mol-2.
- ‘b’ (Volume Correction Term / Excluded Volume / Co-volume): Corrects for the finite volume occupied by the gas molecules themselves.
- Its value depends on the size of the gas molecules.
- A larger ‘b’ value indicates larger molecular size.
- Units of ‘b’: L mol-1 or m3 mol-1.
- The actual volume available for motion is (V−nb).
- ‘a’ (Pressure Correction Term / Attraction Term): Corrects for the intermolecular attractive forces.
- Equation: (P+a(n2/V2))(V−nb)=nRT
- Liquefaction of Gases and Critical Phenomena:
- Andrews’ Isotherms of CO2: Experimental curves showing P-V relationships at different constant temperatures. These experiments led to the concept of critical parameters.
- Critical Temperature (Tc): The maximum temperature above which a gas cannot be liquefied, no matter how high the pressure applied. Above Tc, the substance exists only as a gas.
- Critical Pressure (Pc): The minimum pressure required to liquefy a gas at its critical temperature (Tc).
- Critical Volume (Vc): The volume occupied by one mole of the gas at its critical temperature (Tc) and critical pressure (Pc).
- Relationship with van der Waals constants:
- Tc=8a/27Rb
- Pc=a/27b2
- Vc=3b
- Tc=8a/27Rb
- Significance: Gases with higher critical temperatures (Tc) are easier to liquefy because their intermolecular forces are stronger and they can be liquefied at higher temperatures. (e.g., CO2 has a higher Tc than O2, so CO2 is easier to liquefy).
3. The Liquid State
Liquids represent an intermediate state of matter, where particles are closely packed but retain fluidity.
3.1. Characteristics of Liquids
- Definite Volume, Indefinite Shape: Liquids occupy a fixed volume but take the shape of the container they fill.
- Less Compressible: Liquids are much less compressible than gases but slightly more compressible than solids.
- Moderate Density: Denser than gases, but generally less dense than solids (water is an exception, where ice is less dense than liquid water).
- Fluidity: Particles can slide past one another, allowing liquids to flow.
- Diffusion: Liquids can diffuse into other liquids, though much slower than gases.
3.2. Properties of Liquids
- 1. Vapour Pressure:
- Definition: The pressure exerted by the vapor in equilibrium with its liquid phase at a given temperature. It arises from the dynamic equilibrium where molecules are constantly escaping from the liquid surface into the vapor phase (evaporation) and returning to the liquid phase (condensation).
- Factors Affecting Vapour Pressure:
- Temperature: Vapour pressure increases with increasing temperature. At higher temperatures, a greater fraction of molecules possess sufficient kinetic energy to overcome intermolecular forces and escape into the vapor phase.
- Nature of Liquid (Intermolecular Forces): Liquids with weaker intermolecular forces have higher vapor pressures at a given temperature (they are more volatile). For example, diethyl ether has a higher vapor pressure than water.
- 2. Boiling Point:
- Definition: The temperature at which the vapour pressure of a liquid becomes equal to the external atmospheric pressure. At this temperature, bubbles of vapor form throughout the bulk of the liquid and rise to the surface.
- Normal Boiling Point: The boiling point of a liquid when the external pressure is exactly 1 atmosphere (1 atm or 101.325 kPa).
- Standard Boiling Point: The boiling point of a liquid when the external pressure is exactly 1 bar (100 kPa).
- Factors Affecting Boiling Point:
- External Pressure: Boiling point increases with increasing external pressure (e.g., water boils at less than 100°C on mountains and above 100°C in pressure cookers).
- Intermolecular Forces: Liquids with stronger intermolecular forces require more energy to overcome these attractions and therefore have higher boiling points. (e.g., Water’s high boiling point due to hydrogen bonding).
- 3. Surface Tension (γ):
- Definition: The force acting per unit length perpendicular to an imaginary line drawn on the surface of a liquid, or the energy required to increase the surface area of a liquid by a unit amount. It is the property by virtue of which a liquid surface tends to minimize its surface area, behaving like a stretched membrane.
- Units: Newtons per meter (N/m) in SI units, or dynes per centimeter (dyne/cm) in CGS units. (1 dyne/cm = 10^-3 N/m).
- Cause: Molecules in the bulk of the liquid are attracted equally in all directions by cohesive forces from surrounding molecules. However, molecules at the surface experience a net inward pull towards the bulk of the liquid, leading to a state of tension.
- Factors Affecting Surface Tension:
- Temperature: Surface tension decreases with increasing temperature because increased kinetic energy of molecules weakens the intermolecular forces, reducing the net inward pull.
- Intermolecular Forces: Liquids with stronger intermolecular forces have higher surface tension. (e.g., Water has high surface tension due to hydrogen bonding).
- Presence of Solutes: Impurities can either increase or decrease surface tension. Surfactants (like soaps, detergents) significantly reduce surface tension.
- Applications/Consequences: Spherical shape of liquid drops, wetting and non-wetting phenomena (e.g., water spreading on clean glass vs. beading on waxed surface), capillary action (rise/fall of liquid in narrow tubes), insect walking on water.
- 4. Viscosity (η):
- Definition: The resistance to flow offered by a liquid. It is a measure of the internal friction between adjacent layers of a fluid that are moving relative to each other.
- Units: Pascal-second (Pa s) in SI units, or Poise (P) in CGS units. (1 Pa s = 10 P; 1 poise = 0.1 Pa s).
- Cause: Strong intermolecular forces between liquid layers hinder their relative motion.
- Factors Affecting Viscosity:
- Temperature: Viscosity decreases with increasing temperature as molecules gain kinetic energy and can overcome the frictional forces between layers more easily.
- Intermolecular Forces: Liquids with stronger intermolecular forces have higher viscosity. (e.g., Glycerine is highly viscous due to extensive hydrogen bonding).
- Size and Shape of Molecules: Larger, more complex, or elongated molecules tend to get entangled and generally have higher viscosity compared to smaller, spherical ones.
4. The Solid State
Solids are characterized by their definite shape and volume due to the fixed, orderly arrangement of their constituent particles.
4.1. Characteristics of Solids
- Definite Shape and Volume: Particles are held in fixed positions within a crystal lattice.
- Incompressible: Particles are tightly packed, leaving very little empty space.
- High Density: Generally denser than liquids and gases (exception: ice floats on water).
- Rigidity: Resist deformation.
- Vibrational Motion: Constituent particles can only vibrate about their fixed mean positions; they do not translate or rotate freely.
4.2. Types of Solids
Solids are primarily classified into crystalline and amorphous based on the arrangement of their constituent particles.
- 1. Crystalline Solids:
- Definition: Possess a highly ordered, regular, and repeating three-dimensional arrangement of constituent particles (atoms, ions, or molecules) extending over a long range.
- Characteristics:
- Sharp Melting Point: Melt abruptly and completely at a specific, characteristic temperature.
- Anisotropic: Their physical properties (e.g., electrical conductivity, refractive index, thermal expansion) vary depending on the direction along which they are measured. This is due to the ordered arrangement.
- True Solids: Possess a definite heat of fusion.
- Definite Geometry: Have a characteristic and regular geometrical shape due to the ordered internal structure.
- Cleavage: When cut with a sharp-edged tool, they split into two pieces with smooth, plain surfaces.
- Examples: Sodium Chloride (NaCl), Quartz, Ice, Diamond, most metals.
- Classification based on the nature of intermolecular forces/bonding:
- a. Molecular Solids: Constituent particles are discrete molecules.
- Non-polar Molecular Solids: Held by weak London Dispersion Forces. Low melting points, soft, insulators. (e.g., Solid CO2 (dry ice), solid H2, Iodine (I2)).
- Polar Molecular Solids: Held by dipole-dipole forces. Higher melting points than non-polar molecular solids, soft, insulators. (e.g., Solid HCl, Solid SO2).
- Hydrogen-bonded Molecular Solids: Molecules held by strong hydrogen bonds. Relatively higher melting points than other molecular solids, soft, insulators. (e.g., Ice, solid NH3).
- b. Ionic Solids: Constituent particles are ions (cations and anions). Held by strong electrostatic forces of attraction throughout the crystal lattice. High melting points, hard and brittle, electrical insulators in the solid state but conductors in the molten state or in aqueous solution (due to mobile ions). (e.g., NaCl, MgO, ZnS).
- c. Metallic Solids: Constituent particles are positive metal ions (kernals) immersed in a “sea” of delocalized electrons. Held by strong metallic bonds. High melting points, ductile, malleable, excellent conductors of heat and electricity. (e.g., Iron (Fe), Copper (Cu), Silver (Ag), Gold (Au)).
- d. Covalent (Network) Solids: Constituent particles are atoms, held together by strong covalent bonds forming a continuous, giant three-dimensional network throughout the crystal. Very high melting points, very hard, usually electrical insulators. (e.g., Diamond, Silicon Carbide (SiC), Quartz (SiO2)).
- Graphite Exception: Graphite is a covalent solid with a layered structure. Each carbon atom is sp2 hybridized, forming strong covalent bonds within layers, but layers are held by weak van der Waals forces. It is soft and a good electrical conductor (due to delocalized pi electrons across layers).
- a. Molecular Solids: Constituent particles are discrete molecules.
- 2. Amorphous Solids:
- Definition: Solids where constituent particles are randomly arranged and lack a long-range ordered structure. Their arrangement is more like that of a liquid, but fixed in space.
- Characteristics:
- No Sharp Melting Point: They soften gradually over a range of temperatures before melting.
- Isotropic: Their physical properties are the same in all directions because of the random arrangement of particles.
- Pseudo Solids / Supercooled Liquids: They tend to flow very slowly over long periods (e.g., old window panes thicker at the bottom). They do not have a definite heat of fusion.
- Irregular Shape: When cut with a sharp-edged tool, they break into irregular pieces with uneven surfaces.
- Examples: Glass, Rubber, Plastics, Tar, Amorphous silicon.
4.3. Crystal Lattice and Unit Cell (Basic Concepts)
- Crystal Lattice: The regular, repeating three-dimensional arrangement of constituent particles (atoms, ions, or molecules) in a crystalline solid. Each point in the lattice represents the location of a particle.
- Unit Cell: The smallest repeating three-dimensional portion of a crystal lattice which, when repeated over and over again in different directions, generates the entire crystal lattice. It is the fundamental building block of a crystalline solid.
- Lattice Points: The positions in a crystal lattice occupied by constituent particles.
- Types of Unit Cells (based on particle arrangement within the cell):
- Primitive (Simple Cubic, SC): Particles are present only at the eight corners of the cube.
- Body-Centered Cubic (BCC): Particles are present at the eight corners and one particle at the center of the body of the cube.
- Face-Centered Cubic (FCC): Particles are present at the eight corners and one particle at the center of each of the six faces of the cube.
5. Phase Transitions (Interconversion of States of Matter)
These are physical changes where matter transforms from one state to another, always involving energy absorption or release at constant temperature (phase change temperature).
- Melting (Fusion): Solid → Liquid. This is an endothermic process (absorbs heat, enthalpy of fusion, ΔHfus). Occurs at the melting point.
- Freezing (Solidification): Liquid → Solid. This is an exothermic process (releases heat, −ΔHfus). Occurs at the freezing point (which is the same as the melting point for a pure substance).
- Vaporization (Evaporation/Boiling): Liquid → Gas. This is an endothermic process (absorbs heat, enthalpy of vaporization, ΔHvap).
- Evaporation: Occurs at any temperature below the boiling point, only at the surface.
- Boiling: Occurs at a specific temperature (boiling point) where vapor bubbles form throughout the liquid.
- Condensation (Liquefaction): Gas → Liquid. This is an exothermic process (releases heat, −ΔHvap).
- Sublimation: Solid → Gas directly, without passing through the liquid phase. This is an endothermic process (enthalpy of sublimation, ΔHsub).
- Examples: Dry ice (solid CO2), Naphthalene, Camphor, Iodine.
- Deposition (Desublimation): Gas → Solid directly. This is an exothermic process.
- Triple Point: A unique, specific temperature and pressure at which all three phases (solid, liquid, and gas) of a pure substance can coexist in thermodynamic equilibrium. For water, the triple point is at 0.01$^\circ C$ (273.16 K) and 0.006 atm.
6. Intermolecular Forces (IMFs)
These are the attractive forces that exist between molecules. They are much weaker than intramolecular forces (covalent or ionic bonds within molecules) but are responsible for many macroscopic physical properties of substances (e.g., boiling point, melting point, viscosity, surface tension, solubility).
- 1. Dispersion Forces (London Forces / Instantaneous Dipole-Induced Dipole Forces / Van der Waals forces – general term):
- Nature: These are the weakest type of intermolecular forces. They are universal, meaning they exist between all molecules (polar and non-polar, and noble gas atoms). For non-polar molecules and noble gases, they are the only type of attractive force present.
- Cause: They arise from the temporary, instantaneous fluctuations in electron distribution around an atom or molecule, creating momentary (instantaneous) dipoles. These instantaneous dipoles then induce temporary dipoles in neighboring atoms/molecules, leading to a weak, transient attraction.
- Strength: Increases with:
- Increasing Molecular Size/Molar Mass: Larger molecules have more electrons, which are less tightly held and more easily distorted (more polarizable), leading to stronger instantaneous dipoles.
- Increasing Surface Area: Molecules with larger surface areas have more points of contact for instantaneous dipole interactions, increasing overall strength.
- Impact: Primarily responsible for the boiling points of non-polar compounds (e.g., boiling points of noble gases, hydrocarbons like alkanes).
- 2. Dipole-Dipole Forces:
- Nature: These forces exist between polar molecules (molecules that have permanent dipole moments due to uneven sharing of electrons and asymmetrical structure).
- Cause: Electrostatic attraction between the partially positive end of one polar molecule and the partially negative end of a neighboring polar molecule.
- Strength: Stronger than London Dispersion Forces but weaker than hydrogen bonds.
- Impact: Lead to higher melting and boiling points for polar molecules compared to non-polar molecules of comparable size and molar mass. (e.g., HCl boils at a higher temperature than F2, which has a similar molar mass, due to dipole-dipole forces).
- 3. Hydrogen Bonding:
- Nature: A special, unusually strong type of dipole-dipole interaction. It is the strongest intermolecular force.
- Conditions: Occurs only when a hydrogen atom is covalently bonded to a highly electronegative atom (specifically Fluorine (F), Oxygen (O), or Nitrogen (N)). This creates a highly polarized bond (Hδ+−Xδ−). This δ+ hydrogen then forms an attractive interaction with another highly electronegative atom (F, O, or N) from a neighboring molecule (intermolecular H-bonding) or within the same molecule (intramolecular H-bonding).
- Strength: Much stronger than ordinary dipole-dipole forces but still significantly weaker than true covalent bonds.
- Impact: Leads to many anomalous physical properties:
- Abnormally High Melting and Boiling Points: (e.g., Water (H2O) has a much higher boiling point than H2S, despite H2S being heavier, due to extensive intermolecular H-bonding in water). Similarly for NH3 vs PH3, HF vs HCl.
- Higher Solubility in Water: Substances that can form hydrogen bonds with water are often highly soluble in it (e.g., Alcohols, Sugars).
- Density Anomaly of Water: Ice is less dense than liquid water due to the open, cage-like structure formed by hydrogen bonding in ice.
- Biological Significance: Crucial for maintaining the structure and function of biological macromolecules like DNA (holding base pairs together) and proteins (maintaining secondary and tertiary structures).
- Examples: Water (H2O), Ammonia (NH3), Ethanol (CH3CH2OH), Hydrogen Fluoride (HF).
7. Other States of Matter (Briefly for Awareness)
While solid, liquid, and gas are the primary states studied, chemistry recognizes others:
- Plasma:
- Nature: Often called the “fourth state of matter.” It is a superheated, ionized gas consisting of a mixture of free electrons and positive ions.
- Properties: Electrically conductive, responds strongly to electromagnetic fields.
- Occurrence: Most common state of matter in the universe (stars, lightning), also found in fluorescent lamps and plasma televisions.
- Bose-Einstein Condensate (BEC):
- Nature: A state of matter formed when a gas of bosons (particles with integer spin) is cooled to temperatures incredibly close to absolute zero (nano-Kelvin range).
- Properties: At this extreme temperature, the individual atoms lose their individual identities and condense into the lowest possible quantum state, behaving as a single quantum mechanical wave or “superatom.” Exhibits superfluidity and superconductivity.
- Occurrence: Created in laboratories.