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3 Thermal

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THERMAL EQUILIBRIUM
THERMAL CONCEPTS
MOLECULAR THEORY OF SOLIDS, LIQUIDS AND GASES
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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
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Relative temperature determines direction of energy flow
Absolute temperature is in kelvin, 0 is at absolute 0 – conversion: 𝑇(𝐾) = πœƒ(°πΆ) + 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
𝑄 = π‘šπ‘Δ𝑇
Energy lost by hot substance = energy gained by cold substance
π‘šπ΄ 𝑐𝐴 (𝑇𝐴 − π‘‡π‘šπ‘Žπ‘₯ ) = π‘šπ΅ 𝑐𝐡 (π‘‡π‘šπ‘Žπ‘₯ − 𝑇𝐡 )
PHASE CHANGE
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1. Energy is supplied to solid – increase in internal energy – increase in 𝐸𝐾 π‘Žπ‘›π‘‘ 𝐸𝑃
2. Bonds start to break – only 𝐸𝑃 of molecules is increasing
3. Groups of molecules are free – solid has melted - 𝐸𝐾 starts increasing again – on avg 𝐸𝑃
doesn’t change
4. As it starts to boil the groups of molecules break up – 𝐸𝑃 starts increasing - πΈπ‘˜ constant
5. Once liquid is vaporized πΈπ‘˜ 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
𝑄 = 𝑀𝐿
Energy lost in cooling water = energy gained by ice
π‘šπ‘€π‘Žπ‘‘π‘’π‘Ÿ π‘π‘€π‘Žπ‘‘π‘’π‘Ÿ (π‘‡π‘€π‘Žπ‘‘π‘’π‘Ÿ − π‘‡π‘šπ‘–π‘₯ ) = π‘šπ‘–π‘π‘’ πΏπ‘“π‘’π‘ π‘–π‘œπ‘› + π‘šπ‘–π‘π‘’ π‘π‘€π‘Žπ‘‘π‘’π‘Ÿ π‘‡π‘šπ‘–π‘₯
MODELLING A GAS
PRESSURE
𝑃=
𝐹
𝐴
EQUATION OF STATE FOR AN IDEAL GAS
𝑃𝑉 = 𝑛𝑅𝑇
-
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
𝑛=
𝑁
π‘›π‘’π‘šπ‘π‘’π‘Ÿ π‘œπ‘“ π‘Žπ‘‘π‘œπ‘šπ‘ 
=
𝑁𝐴 π΄π‘£π‘œπ‘”π‘Žπ‘Ÿπ‘‘π‘œ π‘π‘œπ‘›π‘ π‘‘π‘Žπ‘›π‘‘
DIFFERENCES BETWEEN REAL AND IDEAL GASSES
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-
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
𝐸̅𝐾 =
-
3
3𝑅
π‘˜π΅ 𝑇 =
𝑇
2
2 𝑁𝐴
Internal energy of a gas is entirely kinetic thus:
π‘‘π‘œπ‘‘π‘Žπ‘™ π‘–π‘›π‘‘π‘’π‘Ÿπ‘›π‘Žπ‘™ π‘’π‘›π‘’π‘Ÿπ‘”π‘¦ π‘œπ‘“ π‘Ž π‘”π‘Žπ‘  =
𝑝𝑉 = π‘π‘˜π΅ 𝑇
3
π‘π‘˜ 𝑇
2 𝐡
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