Chapter 4 Ideal Gases Flashcards

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1
Q

Amount of Substance

A

-In thermodynamics, the amount of substance is measured in the SI unit ‘mole’
-This has the symbol mol
-The mole is a unit of substance, not a unit of mass
-The mole is defined as:
The SI base unit of an ‘amount of substance’. It is the amount containing as many particles (e.g. atoms or molecules) as there are atoms in 12 g of carbon-12

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2
Q

The Avogadro Constant

A
  • A carbon-12 atom has a mass of:

12 u = 12 × 1.66 × 10-27 = 1.99 × 10-26 kg

  • The exact number for a mole is defined as the number of molecules in exactly 12 g of carbon:

1 mole= 0.012/1.99x10-26= 6.02 x 1023 molecules

  • Avogadro’s constant (NA) is defined as:

The number of atoms of carbon-12 in 12 g of carbon-12; equal to 6.02 × 1023 mol-1

  • For example, 1 mole of sodium (Na) contains 6.02 × 1023 atoms of sodium
  • The number of atoms can be determined if the number of moles is known by multiplying by NA, for example:

2.0 mol of nitrogen contains: 2.0 × NA = 2.0 × 6.02 × 1023 = 1.20 × 1024 atoms

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3
Q

Mole and the Atomic Mass

A
  • One mole of any element is equal to the relative atomic mass of that element in grams
    • E.g. Helium has an atomic mass of 4 – this means 1 mole of helium has a mass of 4 g
  • If the substance is a compound, add up the relative atomic masses, for example, water (H2O) is made up of
    • 2 hydrogen atoms (each with atomic mass of 1) and 1 oxygen atom (atomic mass of 16)
    • So, 1 mole of water would have a mass of (2 × 1) + 16 = 18 g
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4
Q

Molar Mass

A
  • The molar mass of a substance is the mass, in grams, in one mole
    • Its unit is g mol-1
  • The number of moles from this can be calculated using the equation:

no moles= mass(g)/molar mass (g mol-1)

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5
Q

Ideal Gases

A
  • An ideal gas is one which obeys the relation:

pV ∝ T

  • Where:
    • p = pressure of the gas (Pa)
    • V = volume of the gas (m3)
    • T = thermodynamic temperature (K)
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6
Q

Gas molecules move about randomly. what other conditions affect

A
  • temperature
  • momentum
  • pressure
  • volume
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7
Q

Gas molecules move about randomly. what other conditions affect: temperature

A
  • The temperature of a gas is related to the average speed of the molecules:
    • The hotter the gas, the faster the molecules move
    • Hence the molecules collide with the surface of the walls more frequently
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8
Q

Gas molecules move about randomly. what other conditions affect: momentum

A
  • Each collision applies a force across the surface area of the walls
  • The faster the molecules hit the walls, the greater the force on them
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9
Q

Gas molecules move about randomly. what other conditions affect: pressure

A
  • Since pressure is the force per unit area
    • Higher temperature leads to higher pressure
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10
Q

Gas molecules move about randomly. what other conditions affect: volume

A
  • If the volume V of the box decreases, and the temperature T stays constant:
    • There will be a smaller surface area of the walls and hence more collisions
    • This also creates more pressure
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11
Q

greater force per unit area, pressure in an ideal gas is therefore defined by:

A

The frequency of collisions of the gas molecules per unit area of a container

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12
Q

Boyle’s Law

A
  • If the temperature T is constant, then Boyle’s Law is given by:

p ∝ 1/V

  • This leads to the relationship between the pressure and volume for a fixed mass of gas at constant temperature:

P1V1 = P2V2

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13
Q

Charles’s Law

A
  • If the pressure P is constant, then Charles’s law is given by:

V ∝ T

  • This leads to the relationship between the volume and thermodynamic temperature for a fixed mass of gas at constant pressure:

V1/T1 = V2/T2

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14
Q

Pressure Law

A
  • If the volume V is constant, the the Pressure law is given by:

P ∝ T

  • This leads to the relationship between the pressure and thermodynamic temperature for a fixed mass of gas at constant volume:
  • P1/T1 = P2/T2
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15
Q

Ideal Gas Equation

A

pV = nRT

or

pV= NkT

  • An ideal gas is therefore defined as:

A gas which obeys the equation of state pV = nRT at all pressures, volumes and temperatures

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16
Q

The Boltzmann Constant

A
  • The Boltzmann constant k is used in the ideal gas equation and is defined by the equation:

K= R/NA

  • Where:
    • R = molar gas constant
    • NA = Avogadro’s constant
  • Boltzmann’s constant therefore has a value of

K=8.13/6.02x1023=1,38x10-23J K-1

17
Q
  • The Boltzmann constant relates the properties of ..
A
  • microscopic particles (e.g. kinetic energy of gas molecules) to their macroscopic properties (e.g. temperature)
    • This is why the units are J K-1
  • Its value is very small because the increase in kinetic energy of a molecule is very small for every incremental increase in temperature
18
Q

Kinetic Theory of Gases

A
  • Gases consist of atoms or molecules randomly moving around at high speeds
  • The kinetic theory of gases models the thermodynamic behaviour of gases by linking the microscopic properties of particles (mass and speed) to macroscopic properties of particles (pressure and volume)
19
Q

Assumptions of the Kinetic Theory of Gases

A
  • Molecules of gas behave as identical, hard, perfectly elastic spheres
  • The volume of the molecules is negligible compared to the volume of the container
  • The time of a collision is negligible compared to the time between collisions
  • There are no forces of attraction or repulsion between the molecules
  • The molecules are in continuous random motion
  • The number of molecules of gas in a container is very large, therefore the average behaviour (eg. speed) is usually considered
20
Q

Root-Mean-Square Speed

A
  • The pressure of an ideal gas equation includes the mean square speed of the particles:

2>

  • Where
    • c = average speed of the gas particles
    • 2> has the units m2 s-2
21
Q

In order to find the pressure of the gas, the

A
  • velocities must be squared
    • This is a more useful method, since a negative or positive number squared is always positive
22
Q
  • To calculate the average speed of the particles in a gas, take the square root of the mean square speed:
A
  • cr.m.s is known as the root-mean-square speed and still has the units of m s-1
  • The mean square speed is not the same as the mean speed
23
Q

5 Step Derivation of the Kinetic Theory of Gases Equation

A

1.Find the change in momentum as a single molecule hits a wall perpendicularly

2. Calculate the number of collisions per second by the molecule on a wall

3.Find the change in momentum per second

4. Calculate the total pressure from N molecules

5. Consider the effect of the molecule moving in 3D space

24
Q

5 Step Derivation of kinetic theory of gases: No. 1

Find the change in momentum as a single molecule hits a wall perpendicularly

A
  • One assumption of the kinetic theory is that molecules rebound elastically
  • This means there is no kinetic energy lost in the collision
  • If they rebound in the opposite direction to their initial velocity, their final velocity is -c
  • The change in momentum is therefore:

Δp = −mc − (+mc) = −mc − mc = −2mc

25
Q

5 Step Derivation of kinetic theory of gases: No. 2

Calculate the number of collisions per second by the molecule on a wall

A
  • The time between collisions of the molecule travelling to one wall and back is calculated by travelling a distance of 2l with speed c:
  • time between collisions = distance/speed = 2l/c
  • Note: c is not taken as the speed of light in this scenario
26
Q

5 Step Derivation of kinetic theory of gases: No. 3

Find the change in momentum per second

A
  • The force the molecule exerts on one wall is found using Newton’s second law of motion:

Force = rate of change of momentum = ∇p/∇t = 2mc/(2l/c) = mc2/l

  • The change in momentum is +2mc since the force on the molecule from the wall is in the opposite direction to its change in momentum
27
Q

5 Step Derivation of kinetic theory of gases: No. 4

Calculate the total pressure from N molecules

A
  • The area of one wall is l2
  • The pressure is defined using the force and area:

Pressure p = Force/area =(mc2/l) / l2 = mc2 / l3

  • This is the pressure exerted from one molecule
  • To account for the large number of N molecules, the pressure can now be written as:

p= Nmc2/l3

  • Each molecule has a different velocity and they all contribute to the pressure
  • The mean squared speed of c2 is written with left and right-angled brackets 2>
  • The pressure is now defined as:
  • p= Nm2> / l3
28
Q

5 Step Derivation of kinetic theory of gases: No. 5

Consider the effect of the molecule moving in 3D space

A
  • The pressure equation still assumes all the molecules are travelling in the same direction and colliding with the same pair of opposite faces of the cube
  • In reality, all molecules will be moving in three dimensions equally
  • Splitting the velocity into its components cx, cy and cz to denote the amount in the x, y and z directions, c2 can be defined using pythagoras’ theorem in 3D:

c2 = cx2 + cy2 + cz2

  • Since there is nothing special about any particular direction, it can be determined that:

x2> = y2> = z2>

  • Therefore, x2> can be defined as:

x2> = ⅓ x2>

  • The box is a cube and all the sides are of length l
    • This means l3 is equal to the volume of the cube, V
  • Substituting the new values for 2> and l3 back into the pressure equation obtains the final equation:

pV=⅓ Nmx2>

29
Q

Kinetic Theory of Gases equation

A
  • This can also be written using the density ρ of the gas:

p= mass/volume = Nm/V

  • Rearranging the pressure equation for p and substituting the density ρ:

p = ⅓ p2>

30
Q

Average Kinetic Energy of a Molecule

A
  • An important property of molecules in a gas is their average kinetic energy
  • This can be deduced from the ideal gas equations relating pressure, volume, temperature and speed
31
Q

Average Kinetic Energy of a Molecule equation

A
  • Recall the ideal gas equation:

pV = NkT

  • Also recall the equation linking pressure and mean square speed of the molecules:

pV=⅓ Nm2>

  • The left hand side of both equations are equal (pV)
  • This means the right hand sides are also equal:

⅓ Nm2≥ NkT

  • N will cancel out on both sides and multiplying by 3 obtains the equation:

m2> = 3kT

  • Recall the familiar kinetic energy equation from mechanics:

kinetic energy = ½mv2

  • Instead of v2 for the velocity of one particle, 2> is the average speed of all molecules
  • Multiplying both sides of the equation by ½ obtains the average translational kinetic energy of the molecules of an ideal gas:

Ek = ½ m2≥3/2 kT

  • Where:
    • EK = kinetic energy of a molecule (J)
    • m = mass of one molecule (kg)
    • 2> = mean square speed of a molecule (m2 s-2)
    • k = Boltzmann constant
    • T = temperature of the gas (K)
32
Q
  • A key feature of this equation is that the mean kinetic energy of an ideal gas molecule is proportional to its thermodynamic temperature
A

Ek ∝ T

33
Q

Translational kinetic energy is defined as

A

The energy a molecule has as it moves from one point to another

  • A monatomic (one atom) molecule only has translational energy, whilst a diatomic (two-atom) molecule has both translational and rotational energy