C15 Ideal Gases Flashcards

1
Q

SI unit of measurement for the amount of a substance

A

The Mol (Mole)

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2
Q

Define ‘one mole’

A

The amount of substance that contains are many elementary entities as there are atoms in 12g of carbon-12.

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3
Q

State Avogrado’s Constant

A

6.022 x 10^23

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4
Q

Formula to calculate number of particles in a substance, N

A

N = n x N(a)

n = number of moles
N(a) = Avogadro’s Constant

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5
Q

Formula to calculate the molar mass of a substance, M

A

M = m / n

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6
Q

State assumptions made in the kinetic model for an ideal gas

A
  • The gas contains a very large number of particles moving in random directions with random speeds.
  • The particles of the gas occupy a negligible volume compared with the volume of the gas.
  • The collisions of the particles with each other and the container walls are perfectly elastic (no KE lost).
    The time of the collisions between the particles is negligible compared to the to the time between the collisions.
  • Electrostatic forces between particles are negligible except during collisions.
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7
Q

How does the speed/velocity/momentum of an atom change when it bounces off a boundary at?

A
  • Speed remain the same, as it is a scalar.
  • Velocity is the negative speed, as the direction is opposite.
  • Change in momentum = -2mu
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8
Q

State Boyle’s Law and conditions

A

P ∝ 1/V or pV = constant
Assuming constant temperature and mass of the gas.

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9
Q

State the relationship between pressure and temperature and conditions

A

p ∝ T or p/T = constant
Assuming the volume and the mass of the gas remain constant.
T is always measured in kelvin

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10
Q

Combining the gas laws formula and how it can be applied

A
  • pV / T = constant
  • Can be used when conditions are changing from an initial state to a final state
  • P1V1 / T1 = P2V2 / T2
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11
Q

State the equation of state for an ideal gas

A
  • For one mole of an ideal gas, the constant in the combined temperature is the molar gas constant, R
  • pV / T = nR or pV = nRT
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12
Q

State the value/unit for R (molar gas constant)

A

8.31 J K-1 mol-1

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13
Q

Describe the graph of pV against T

A
  • This produces a straight line through the origin, as pV ∝ T
  • By comparing y = mx + c and pV = nRT
  • Gradient: nR
  • The greater the number of moles, the steeper the line.
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14
Q

Average velocity of particles in a gas

A

It would be 0 m/s, as the particles all move in random directions at different speeds, cancelling out.

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15
Q

Average velocity of particles in a gas

A

It would be 0 m/s, as the particles all move in random directions at different speeds, cancelling out.

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16
Q

How do we determine r.m.s speed

A
  • The velocity of each particle is squared, and the average of these squares is calculated.
  • The square root of the average is taken.
17
Q

Formula for pressure at the microscopic level

A

pV = 1/3 Nmc(squared bar)

where:
N = number of particles in the gas
m = mass of each particle
c (squared bar) = mean square speed of the particles

18
Q

Deriving pV = 1/3 Nmc(squared bar)

A
  • Consider a single gas particle, mass m, velocity c, in a cube container of sides L.
  • The time t between collisions is 2L / c
  • Force = change in momentum / time
  • Force = 2mc x c / 2L = mc(squared) / L
  • If there are N particles, average force = mc(squared bar) / L, where c(squared bar) = mean square speed
  • On average, about 1/3 of the particles are moving between opposite faces.
  • CSA = L^2
  • Force = mc(squared bar) x N x 1/3
  • p = Nmc(squared bar) / 3L x 1 / L(squared)
  • L(cubed) = volume
  • pV = 1/3Nmc(squared bar)
19
Q

What is the Maxwell-Boltzmann distribution?

A
  • In a container, gas particles will all be moving at different speeds, from very fast to very slow.
  • The range of speeds the particles can take at a given temperature is the Maxwell-Boltzmann distribution.
20
Q

How does changing the temperature of a gas affect the Maxwell-Boltzmann distribution?

A
  • The hotter that gas becomes, the greater the range of speeds.
  • The modal speed and r.m.s increases.
  • The distribution becomes more spread out.
21
Q

State the Boltzmann constant

A

k = R / N(a)
1.38 x 10^-23 J/K

22
Q

The second equation of the state of an ideal gas, by substituting the Boltzmann constant

A

pV = nRT —> pV = nKN(a)T
Number of particles in the gas, N = n x N(a)
pV = NkT

23
Q

Equation that relates the mean KE of a particle to the absolute temperature of the gas

A

1/3Nmc(squared bar) = NkT
Cancel out N, sub out 2/3
1/2mc(squared bar) = 3/2 kT

24
Q

Relationship between temperature and kinetic energy and conditions

A

E(k) ∝ T
Assuming the temperature is measured in kelvin.

25
Q

Internal energy of an ideal gas

A
  • In an ideal gas, there are negiblible electrostatic forces between particles unless during a collision.
  • This means the internal energy of a particle in an ideal gas is entirely its kinetic energy.
  • Doubling temperature doubles K(e), so internal energy.