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STATES OF MATTER -Presented by SHRABANTI HALDER Class-XI A
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Page 1: States of matter

STATES OF MATTER

-Presented bySHRABANTI HALDER

Class-XI A

Page 2: States of matter

THREE STATES OF MATTER Some Characteristics of Gases, Liquids and Solids and the

Microscopic Explanation for the Behavior

assumes the shape and volume of its container

particles can move past one another

assumes the shape of the part of the container which

it occupies particles can move/slide

past one another

retains a fixed volume and shape 

rigid - particles locked into place

compressible lots of free space between

particles

not easily compressible little free space between

particles

not easily compressible little free space between

particles

flows easily particles can move past one

another

flows easily particles can move/slide

past one another

does not flow easily rigid - particles cannot

move/slide past one another

Gas Liquids Solids

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INTERMOLECULAR FORCES

Intramolecular forces are attractive forces between molecules.They hold atoms together in a molecule.

INTERMOLECULAR Vs INTRAMOLECULAR41 KJ to vaporize 1 mole of water (inter)930 KJ to break all O-H bonds in 1 mole of water (intra)

Measure of intermolecular force

boiling point

melting point

ΔHvap ΔHsub ΔHfus

Generally, Intermolecular forces are muchweaker thanIntramolecular forces.

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TYPES OF INTERMOLECULAR FORCES

DISPERSION FORCES OR LONDON FORCES

The London dispersion force is

the weakest intermolecular force. The London dispersion force is a temporary attractive force that results when the electrons in two adjacent atoms occupy positions that make the atoms form temporary dipoles. This force is sometimes called an induced dipole-induced dipole attraction. London forces are the attractive forces that cause nonpolar substances to condense to liquids and to freeze into solids when the temperature is lowered sufficiently..

Page 8: States of matter

DIPOLE - DIPOLE FORCES Dipole-dipole forces are attractive forces between

the positive end of one polar molecule and the negative end of another polar

molecule. Dipole-dipole forces have strengths that range from 5 kJ to 20 kJ per

mole. They are much weaker

than ionic or covalent bonds and have a significant effect only when the molecules involved are close

together (touching or almost touching).

Page 9: States of matter

INDUCED - DIPOLE FORCES

Ion – induced dipole forces An ion-induced dipole attraction

is a weak attraction that results when the approach of an ion induces a dipole in an atom or in a nonpolar molecule by disturbing the arrangement of electrons in the nonpolar species.

Dipole – Induced Dipole Forces A dipole-induced dipole

attraction is a weak attraction that results when a polar molecule induces a dipole in an atom or in a nonpolar molecule by disturbing the arrangement of electrons in the nonpolar species.

Page 10: States of matter

HYDROGEN BOND

The hydrogen bond is a special dipole-dipole interaction between the

hydrogen atom in a polar N-H, O-H or F-H bond and an electronegative

O, N or F atom.

A – H ----B or A – H ----A A and B are O, N and F

Page 11: States of matter

BOYLE’S LAW (Pressure – Volume Relationship)

According to Robert Boyle’s Law, at constant temperature, the

pressure of a fixed amount of gas varies inversely with its volume.

GAS LAWS

pv = constant pv = k

Page 12: States of matter

CHARLE’S LAW (Temperature – Volume Relationship)

Charle’s Law states that pressure remaining constant, the

volume of a fixed mass of a gas is directly proportional

to it’s absolute temperature.

Page 13: States of matter

GAY LUSSAC’S LAW (Pressure – Temperature Relationship)

Gay Lussac’s law states that at constant volume, pressure of a

fixed amount of a gas varies directly with the temperature.

Page 14: States of matter

AVAGADRO LAW (Volume – Amount Relationship)

It states that equal volumes of all gases under the same conditions

of temperature and pressure contain equal number of molecules.

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Ideal gas equation is a relation between four variables and it describes the

state of any gas, therefore, it is also called equation of state.

IDEAL GAS EQUATIONIDEAL GAS EQUATION

Combined gas law

Page 16: States of matter

This law states that the total pressure exerted by the mixture of non-reactive

gases is equal to the sum of the partial pressures of individual gases.

DALTON’S LAW OF PARTIAL DALTON’S LAW OF PARTIAL PRESSUREPRESSURE

Page 17: States of matter

A gas is composed of particles in constant motion.The average kinetic energy depends on temperature, the higher the temperature, the higher the kinetic energy and the faster the particles are moving.Compared to the space through which they travel, the particles that make up the gas are so small that their volume can be ignored.The individual particles are neither attracted to one another nor do they repel one another.When particles collide with one another (or the walls of the container) they bounce rather than stick. These collisions are elastic; if one particle gains kinetic energy another loses kinetic energy so that the average remains constant.

KINETIC MOLECULAR THEORY ON GASES

The Assumptions of Kinetic Molecular Theory:

Page 18: States of matter
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A gas which obeys the gas laws and the gas equation PV = nRT strictly at all temperatures and pressures is said to be an ideal gas. The molecules of ideal gases are assumed to be volume less points with no attractive forces between one another. But no real gas strictly obeys the gas equation at all temperatures and pressures. Deviations from ideal behaviour are observed particularly at high pressures or low temperatures. The deviation from ideal behaviour is expressed by introducing a factor Z known as compressibility factor in the ideal gas equation. Z may be expressed as Z = PV / nRT  •       In case of ideal gas, PV = nRT so, Z = 1  •       In case of real gas, PV ≠ nRt  so,Z ≠ 1 Thus in case of real gases Z can be < 1 or > 1  (i)   When Z < 1, it is a negative deviation. It shows that the gas is more compressible

than expected from ideal behaviour.

(ii)   When Z > 1, it is a positive deviation. It shows that the gas is less compressible than expected from ideal behaviour.

BEHAVIOUR OF REAL GASES : DEVIATION FROM IDEAL GAS BEHAVIOUR

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Causes of deviation from ideal behaviour  The causes of deviations from ideal behaviour may be

due to the following two assumptions of kinetic theory of gases.

There are 

The volume occupied by gas molecules is negligibly small as compared to the volume occupied by the gas.The forces of attraction between gas molecules are negligible.

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Atoms and molecules are never truly ideal because they all interact with other gas particles; weak attractions between separate gas particles are known as intermolecular attractions or van der Waals forces after the chemist who proposed a correction to the ideal gas law to calculate pressure of a real gas. Van der Waals proposed that the ideal gas equation could be corrected for real gas behavior by subtracting the effective gas particle volume from the volume of the container and by correcting for intermolecular attractions:

VAN DER WAALS EQUATION

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VAPOUR PRESSURE The pressure exerted by the vapours in equillibrium

wiyh liquids form of the same substance is called vapour

pressure of the liquid.

PROPERTIES OF LIQUIDS

Page 23: States of matter

SURFACE TENSION Surface tension is the force acting per unit length

perpendicular to the line drawn on the surface of the liquid.

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VISCOSITY

Viscosity of a liquid is measure of its resistance to flow. It is related to

inter molecular force of attraction ; stronger these forces, greater the viscosity.

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CHAPTER

COMPLETED