Thermal Flashcards
Phases of matter
Solid:
- Particles are closely packed in a fixed lattice structure, held by strong intermolecular forces.
- Particles can only vibrate about fixed positions and have low energy.
- Solids have high density and are incompressible.
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Liquid:
- Particles are closely packed, randomly arranged, and held by weaker intermolecular forces than solids.
- Particles can flow past each other and have higher energy than solids but lower than gases.
- Liquids have a fixed volume, take the shape of their container, and are difficult to compress.
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Gas:
- Particles have negligible intermolecular forces, are randomly arranged, and are far apart.
- Particles move freely in all directions at various speeds and have higher energy than solids and liquids.
- Gases take the shape of their container, have no fixed volume, are compressible, and have the lowest densities.
Brownian motion
- The random movement of small particles suspended in a liquid or gas, caused by collisions with faster-moving atoms or molecules.
- Supports the idea of molecular motion and explains the concept of pressure in gases.
- Smaller molecules affect larger particles due to their high speeds and momentum transfer during collisions.
Energy during change of phase
Phase Changes:
- During phase changes, energy increases or decreases electrostatic potential energy instead of kinetic energy, so temperature remains constant.
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Melting or Boiling:
- Energy breaks intermolecular bonds, increasing electrostatic potential energy and moving molecules further apart.
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Freezing or Condensation:
- Energy forms bonds, decreasing electrostatic potential energy and moving molecules closer together.
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Kinetic Energy:
- Stays constant, indicating no temperature change during a phase transition.
Specific heat capacity
Amount of energy needed to raise the temperature of unit mass (1 kg) of a substance by 1 K (unit temp)
Internal energy
- The sum of the randomly distributed kinetic and potential energies of atoms or molecules within a substance.
- ΔU ∝ ΔT: Internal energy is proportional to temperature change.
- Stronger intermolecular forces result in higher potential energy.
Thermal equilibrium
Heat Flow and Thermal Equilibrium:
- Heat flows from a hotter object to a colder one until both reach the same temperature (thermal equilibrium).
- Thermal equilibrium occurs when two substances in contact no longer exchange heat energy and reach the same temperature.
- The final temperature depends on the initial temperature difference between the objects (e.g., ice cubes melting in room temperature water).
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Energy Balance:
- Energy lost by hotter object = Energy gained by colder object.
- For ice:
Energy gained = ml + mc(T -T1) - For hot drink:
Energy lost = mc(T2 - T):
Specific Latent Heat
Specific Latent Heat:
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Fusion:
- Energy required to convert 1 kg of solid to liquid with no temperature change.
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Vaporisation:
- Energy required to convert 1 kg of liquid to gas with no temperature change.
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Key Points:
- Evaporating 1 kg of water requires seven times more energy than melting 1 kg of ice.
- Ice melting: Increases molecular separation.
- Boiling water: Fully separates molecules, breaking all intermolecular forces.
Triple-Point
The specific temperature and pressure where a substance exists as a solid, liquid, and gas simultaneously.
Gas Laws
Boyle’s Law:
- p ∝ V-1 (at constant temperature).
- If temperature increases, the graph is further from the origin, and vice versa.
- The area under the graph represents energy.
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Pressure Law:
- p ∝ T
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Charles’s Law:
- V ∝ T
Avogadro Constant
Mole:
- The SI base unit for the amount of substance, defined as the amount containing as many particles (e.g., atoms or molecules) as there are in 12 g of carbon-12.
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Avogadro’s Constant (Na):
- The number of atoms in 12 g of carbon-12.
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Equation:
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N = n × Na
Where: - n: Number of moles
- Na: Avogadro’s Constant
- N: Number of particles
Molar mass
Molar Mass
- The mass of one mole of a substance, measured in grams per mole (g mol⁻¹).
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Equation:
- n × M = m
Where:
- n: Number of moles
- m: Mass of the substance (g)
- M: Molar mass (g mol⁻¹)
Molar Gas Constant (R)
- The constant in the equation pVT-1 depends on the amount of gas (measured in moles, n).
- Equation: constant=nR
- Relates energy to temperature in thermal physics for a mole of particles at a given temperature.
Boltzmann’s constant
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Boltzmann constant (kB) links the average kinetic energy of particles in a gas to its temperature.
- kB = R / Nₐ
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Derivation of nR = NkB:
- kB = R / Nₐ
- R / (N/n) = kB
- nR/N = kB
- nR= NkB
Kinetic Theory of Gases (R.A.V.E.D.)
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R | Random:
- A large number of gas particles move randomly in straight lines until they collide with each other or the container walls.
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A | Attraction:
- No intermolecular forces between particles except during collisions.
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V | Volume:
- Negligible volume of particles compared to the volume of the gas.
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E | Elastic:
- Elastic collisions: Collisions between particles and with container walls are perfectly elastic.
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D | Duration:
- Negligible time spent on each collision compared to the time between collisions.
Pressure in terms of the kinetic theory of gases and Newtonian thoery
Gas Particle Motion:
- Gas particles move randomly with constant velocities and no intermolecular forces, following Newton’s 1st law (objects in motion stay in motion unless acted upon).
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Collisions and Force:
- When particles collide with the walls of the container, they exert a force on the wall, and the wall exerts an equal and opposite force (Newton’s 3rd law).
- The force on the wall is calculated using Newton’s 2nd law (force = rate of change of momentum).
- The momentum change during a collision (from mu to -mu) results in a force proportional to the particle’s mass and velocity.
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Pressure:
- Although each particle exerts a tiny force, billions of particles create a combined force, leading to a steady, uniform pressure on the walls.
- Pressure results from many collisions between particles and the container walls.
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Equation:
Pressure = (Rate of momentum ÷ area) × number of particles
Root Mean Square
Gas Particle Motion:
- Gas particles move in random directions, resulting in a net velocity of zero.
- Squaring the velocities ensures all values are positive, avoiding cancellation.
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Root-Mean-Square Speed (crms):
- crms =√mean(c2).
- Provides the average speed of particles by taking the square root of the mean square speed.
Maxwell-Boltzmann distribution
Maxwell-Boltzmann Distribution:
- Shows the range of kinetic energies of gas particles, with most particles moving at moderate speeds, and fewer at very high or low speeds.
- The curve starts at (0, 0) because no molecules have zero energy, and it peaks at the most-probable energy/speed.
- Kinetic energy is proportional to the square of speed, so the distribution can also represent particle speeds.
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Effect of Temperature:
- As temperature increases, the average speed, most-probable speed, and maximum speed all increase, and the curve becomes broader and flatter.
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Collisions and Energy:
- Collisions between particles redistribute momentum and energy, creating a skewed bell-shaped curve while maintaining the gas’s total energy.
Kinetic energy of a molecule
Kinetic Theory of Gases:
- Connects the microscopic properties of gas particles (e.g., mass and speed) to their macroscopic properties (e.g., pressure and volume).
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Key Equations:
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1/3N mc2 = N kbT where:
- m = mass of one molecule.
- c = speed of molecules.
- kb = Boltzmann constant.
- T = temperature.
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Pressure:
pressure = 1/3ρc2 where Nm/V = ρ -
Rearranged for Energy:
1/2mc2 = 3/2kbT
Internal energy of an ideal gas
Internal Energy of an Ideal Gas:
- Entirely due to the kinetic energy of its particles.
- Electrostatic forces between particles are negligible except during collisions, meaning there is no electrostatic potential energy.
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Heating the Gas:
- When the container is heated, gas molecules move faster, increasing kinetic energy and internal energy.
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Change in Internal Energy (∆U):
- Equal to the total kinetic energy (Ek) of all the particles.
Kinetic theory equation derivation
Force Exerted by a Molecule on the Wall:
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F = -2mv / t
where:- m = mass of molecule.
- v = velocity.
- t = time between collisions.
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Time Between Collisions (t):
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t = 2L / v
, where L = length of the container.
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Pressure (p):
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p = F/A,
where A = area of the wall. - Substituting F and t :
p = mv2 / V,
where V = volume of the container V = L × A
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For N Molecules:
- p = (Nm × v2) / 3V where v2 = mean square velocity.
Absolute Zero
- The lowest possible temperature, defined as 0 K or -273°C.
- At absolute zero, molecules have zero kinetic energy, and no further energy can be removed from the system.