Thermal Physics Flashcards

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1
Q

Internal Energy

A

The sum of the randomly distributed kinetic and potential energies of all its particles.

Some particles move faster than others so kinetic energy is randomly distributed.

They also have randomly distributed potential energies depending on their relative position.

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2
Q

Specific Heat Capacity

A

The energy needed to raise the temperature of unit mass of a substance by 1K without change of state.

Q = m c ςT

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3
Q

Specific Latent Heat

A

The energy required to change the state of a unit mass of a substance without a change in temperature

Energy change = mass of substance changed x specific latent heat

Q = m l

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4
Q

Latent Heat of Fusion

A

The amount of heat required to convert a unit mass of a solid into a liquid without a change in temperature

e. g. Ice to water (melting)
1. Energy supplied
2. Temperature increases
3. Particles gain energy
4. Temperature stops increasing and change of state occurs

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5
Q

Latent Heat of Vaporisation

A

The amount of heat required to convert a unit mass of a liquid into a vapor without a change in temperature

  1. Energy supplied
  2. Temperature increases
  3. Particles gain energy
  4. Temperature stops increasing and change of state occurs
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6
Q

Energy Changes between Particles

A

For a closed system, the total internal energy is constant.

Energy is constantly transferred through particle collisions, but the total internal energy doesn’t change.

The internal energy can be increased by heating or cooling a system, or by doing work e.g. changing its shape

If one of these changes occurs, the average kinetic or potential energy of the particles will change.

When a substance changes state, its internal energy changes but its kinetic energy stays the same, as only the potential energy is changed.

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7
Q

Continuous Flow Calorimeter

A

Continuous-Flow Heating Calorimeter

  • when a fluid flows continuously over a heating element
  • as it flows, energy is transferred to the fluid
  1. Allow water to flow at a steady rate until the water out is at a constant temperature
  2. Record the flow rate of the water and the time taken for the experiment
  3. Measure the temperature difference
  4. Record the current and potential difference
  5. Energy supplied Q = mc ςT + H (H is the heat lost to surroundings)

Specific heat capacity of the liquid (c) = [Q2 – Q1]/(m2 – m1)(θ1 – θo)

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8
Q

Finding the Specific Heat Capacity

A
  1. Weigh the substance and record its mass, m
  2. Record the initial temperature shown on the thermometer
  3. Switch on the heating element and the joulemeter
  4. After a certain amount of time, turn the heating element off
  5. Continue to watch the thermometer in case temperature continues to rise
  6. Record the maximum temperature
  7. Record the energy on the joulemeter
  8. Calculate the specific heat capacity
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9
Q

The Avogadro Constant

A

The avogadro constant is the number of atoms in exactly 12g of the isotope carbon 12.

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10
Q

Amount of Substance

A

The quantity of a substance measured in moles, n.

N = n x Na

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11
Q

Molar Mass

A

The molar mass of a substance is equal to the mass of one mole of the substance.

moles = mass/Mr

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12
Q

The Ideal Gas Equation

A

Combining all three gas laws for a constant mass of gas gives:

pV = nRT

pV/T = a constant

n = number of moles of the gas

R = molar gas constant (8.31)

T = temperature measured in kelvin

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13
Q

Boyle’s Law

A

P1V1 = P2V2

As pressure goes up, the volume goes down (temperature is kept constant):

If the volume of a container decreases, the rate at which particles collide with the walls increases, resulting in increased pressure.

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14
Q

Charles’ Law

A

V1/T1 = V2T2

As temperature increases, the volume increases (pressure is constant):

When air is heated, the particles will gain kinetic energy and there will be more frequent collisions on the walls of the container, forcing it to expand.

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15
Q

Pressure Law

A

P1/T1 = P2/T2

As temperature increases, the pressure increases (volume is constant):

When the temperature increases, the particles gain kinetic energy and collide more, exerting more force, and hence more pressure on the walls of the container.

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16
Q

Brownian Motion

A

The random motion of particles is a result of collisions with fast, randomly moving particles in a fluid.

Einstein explained that the pollen grains that Brownian noticed moving randomly were being moved by individual water molecules:

Heavier particles are moved with Brownian motion by smaller, lighter particles travelling at high speeds

This is evidence that the air is made up of tiny atoms or molecules moving quickly.

The Maxwell Boltzmann Curve demonstrates the distribution of kinetic energy between particles:

17
Q

Maxwell Boltzmann Distribution

A

Shows the number of particles with a certain speed:

Area under the graph = number of particles

Boltzmann’s constant, k is equivalent to R/Na (molar gas constant/avogadro’s constant)

k = 1.38 x 10-23 JK-1

pV = NkT ⇒ equation of state of an ideal gas

18
Q

Work Done In Energy Transfer

A
  1. For a gas to expand or contract at constant pressure, work is done as there is a transfer of energy
  2. When heat is added, it will expand.
  3. When heat is removed, it will contract as heat is transferred back to the surroundings

The work done in changing the volume of a gas at a constant pressure is equal to:

work done = pςV

19
Q

Deriving the Kinetic Theory Equation

A

Kinetic theory links temperature to the speed of the molecules in the gas:

Increasing Pressure

  1. Particles with a greater mass, have a greater force of collision, so greater pressure is exerted
  2. Higher temperature particles move faster and have a greater force of impact and a greater number of impacts
  3. Greater number of particles leads to a greater number of collisions
  4. When the particles collide with the end of a box, the force on the wall is

Force on wall = mv2/x

Pressure = force on wall/area of wall

Pressure = mv2/V

When considering how many molecules, there are N times as many collisions for N molecules

Pressure = Nmv2/V

On average, a 1/3 of the molecules are travelling in each direction

Pressure = 1/3 Nmv2/V

All the molecules are moving at different speeds

pV = 1/3 Nmv2

20
Q

Kinetic Theory Of Gases Assumptions

A
  • Gas has zero volume at zero temperature so the volume of the molecules is negligable
  • Gas has zero pressure at zero temperature so thermal energy is its source of kinetic energy
  • The gas has atoms or molecules which behave as elastic spheres with no long range intermolecular forces.
21
Q

The Boltzmann Constant, K

A

Number of molecules: N = n x NA

n = N/NA

Ideal Gas Equation: pV = nRT

pV = NRT/NA

22
Q

Ideal Gas Definition

A
  • negligable volume
  • collisions are elastic
  • gas cannot be liquified
  • no interactions between molecules (except in collisions)
  • gas obeys the ideal gas law, boyle’s law, pressure law, charles’ law