THERMAL EQUILIBRIUM THERMAL CONCEPTS MOLECULAR THEORY OF SOLIDS, LIQUIDS AND GASES - All matter is made of atoms Solids – fixed volume, fixed shape, atoms are in a solid lattice, limited movement - vibration, Liquids – fixed volume, can change shape, vibrating and molecules can slide over each other Gases – expand to fill a container, no fixed positions, move freely TEMPERATURE AND ABSOLUTE TEMPERATURE - Relative temperature determines direction of energy flow Absolute temperature is in kelvin, 0 is at absolute 0 – conversion: π(πΎ) = π(°πΆ) + 273 INTERNAL ENERGY Internal Energy - Total of the potential energy and the random kinetic energy of all the particles in a substance Kinetic energy is due to movement of particles, potential energy due to intermolecular forces Do not use thermal energy in descriptions – use internal energy and energy transferred due to temperature differences SPECIFIC HEAT CAPACITY Specific Heat Capacity - The amount of energy required to raise the temperature of 1kg of substance by 1K π = ππΔπ Energy lost by hot substance = energy gained by cold substance ππ΄ ππ΄ (ππ΄ − ππππ₯ ) = ππ΅ ππ΅ (ππππ₯ − ππ΅ ) PHASE CHANGE - 1. Energy is supplied to solid – increase in internal energy – increase in πΈπΎ πππ πΈπ 2. Bonds start to break – only πΈπ of molecules is increasing 3. Groups of molecules are free – solid has melted - πΈπΎ starts increasing again – on avg πΈπ doesn’t change 4. As it starts to boil the groups of molecules break up – πΈπ starts increasing - πΈπ constant 5. Once liquid is vaporized πΈπ starts to increase again As a substance changes phase the temperature remains constant SPECIFIC LATENT HEAT Latent Heat - The energy required to achieve a change of phase Specific Latent Heat of Fusion (melting) - Energy required to change the phase of 1kg of substance from a solid to liquid without a temperature change Specific Latent Heat of Vaporization (boiling) - Energy required to change the phase of 1 kg of substance from liquid to gas without a temperature change. Thermal Equilibrium - When the rate of flow of heat from A to B is equal to that from B to A when they are at the same temperature π = ππΏ Energy lost in cooling water = energy gained by ice ππ€ππ‘ππ ππ€ππ‘ππ (ππ€ππ‘ππ − ππππ₯ ) = ππππ πΏππ’π πππ + ππππ ππ€ππ‘ππ ππππ₯ MODELLING A GAS PRESSURE π= πΉ π΄ EQUATION OF STATE FOR AN IDEAL GAS ππ = ππ π - Gas Laws – graphs KINETIC MODEL FOR AN IDEAL GAS Kinetic Model of an Ideal Gas - Gas consists of many small particles in constant random motion ο· Each molecule has negligible volume ο· At any moment as many molecules are moving in one direction as in any other ο· Molecules undergo perfectly elastic collisions - momentum is reversed ο· Energy is entirely kinetic - no intermolecular forces between molecules ο· Duration of a collision is negligible ο· Each molecule produces a force on the wall of the container ο· Forces of individual molecules will average out to produce a uniform pressure throughout MOLE, MOLAR MASS AND THE AVOGADRO CONSTANT Mol - The amount of substance that has the same number of particles as there are neutral atoms in 12 grams of carbon 12. Avogadro Constant – Number of molecules in 1 mol of gas. 6.02 × 1023 Molar Mass – The mass of one mol of substance π= π ππ’ππππ ππ ππ‘πππ = ππ΄ π΄π£ππππππ ππππ π‘πππ‘ DIFFERENCES BETWEEN REAL AND IDEAL GASSES - - An ideal gas is one that follows all gas laws Real gasses have some intermolecular forces, don’t have negligible volume, collisions are not always perfectly elastic Real gasses approximate ideal gasses at high temperature and low pressure πΈΜ πΎ = - 3 3π ππ΅ π = π 2 2 ππ΄ Internal energy of a gas is entirely kinetic thus: π‘ππ‘ππ πππ‘πππππ ππππππ¦ ππ π πππ = ππ = πππ΅ π 3 ππ π 2 π΅