Thermal Flashcards

1
Q

Phases of matter

A

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.

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2
Q

Brownian motion

A
  • 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.
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3
Q

Energy during change of phase

A

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.
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4
Q

Specific heat capacity

A

Amount of energy needed to raise the temperature of unit mass (1 kg) of a substance by 1 K (unit temp)

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5
Q

Internal energy

A
  • 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.
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6
Q

Thermal equilibrium

A

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):
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7
Q

Specific Latent Heat

A

Specific Latent Heat:

  1. Fusion:
    • Energy required to convert 1 kg of solid to liquid with no temperature change.
  2. 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.
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8
Q

Triple-Point

A

The specific temperature and pressure where a substance exists as a solid, liquid, and gas simultaneously.

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9
Q

Gas Laws

A

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
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10
Q

Avogadro Constant

A

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:

  • N = n × Na
    Where:
  • n: Number of moles
  • Na: Avogadro’s Constant
  • N: Number of particles
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11
Q

Molar mass

A

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)

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12
Q

Molar Gas Constant (R)

A
  • 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.
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13
Q

Boltzmann’s constant

A
  • Boltzmann constant (kB) links the average kinetic energy of particles in a gas to its temperature.
    • kB = R / Nₐ
  • Derivation of nR = NkB:
    • kB = R / Nₐ
    • R / (N/n) = kB
    • nR/N = kB
    • nR= NkB
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14
Q

Kinetic Theory of Gases (R.A.V.E.D.)

A
  1. R | Random:
    • A large number of gas particles move randomly in straight lines until they collide with each other or the container walls.
  2. A | Attraction:
    • No intermolecular forces between particles except during collisions.
  3. V | Volume:
    • Negligible volume of particles compared to the volume of the gas.
  4. E | Elastic:
    • Elastic collisions: Collisions between particles and with container walls are perfectly elastic.
  5. D | Duration:
    • Negligible time spent on each collision compared to the time between collisions.
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15
Q

Pressure in terms of the kinetic theory of gases and Newtonian thoery

A

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.
  • Equation:
    Pressure = (Rate of momentum ÷ area) × number of particles
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16
Q

Root Mean Square

A

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.
17
Q

Maxwell-Boltzmann distribution

A

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.
18
Q

Kinetic energy of a molecule

A

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:

  1. 1/3N mc2 = N kbT where:
    • m = mass of one molecule.
    • c = speed of molecules.
    • kb = Boltzmann constant.
    • T = temperature.
  2. Pressure:
    pressure = 1/3ρc2 where Nm/V = ρ
  3. Rearranged for Energy:
    1/2mc2 = 3/2kbT
19
Q

Internal energy of an ideal gas

A

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.
20
Q

Kinetic theory equation derivation

A

Force Exerted by a Molecule on the Wall:

  • F = -2mv / t
    where:
    • m = mass of molecule.
    • v = velocity.
    • t = time between collisions.

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Time Between Collisions (t):

  • t = 2L / v
    , where L = length of the container.

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Pressure (p):

  • 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.
21
Q

Absolute Zero

A
  • 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.