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 as 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 its 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 (for an ideal gas)

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.