Ideal Gas Law and Gas Properties

Master the ideal gas law, gas law calculations, partial pressures, kinetic molecular theory, and real gas behavior.

Ideal Gas Law and Gas Properties

The Ideal Gas Law

The most important equation in gas chemistry:

PV=nRTPV = nRT

Where:

  • PP = pressure (usually atm, but can be kPa, mmHg, torr)
  • VV = volume (usually L)
  • nn = number of moles
  • RR = ideal gas constant
  • TT = temperature (must be in Kelvin!)

Gas Constant (R) Values

Most common:

R=0.0821L\cdotpatmmol\cdotpKR = 0.0821 \frac{\text{Lยทatm}}{\text{molยทK}}

Other values (less common):

R=8.314Jmol\cdotpK=8.314kPa\cdotpLmol\cdotpKR = 8.314 \frac{\text{J}}{\text{molยทK}} = 8.314 \frac{\text{kPaยทL}}{\text{molยทK}}

R=62.4L\cdotpmmHgmol\cdotpKR = 62.4 \frac{\text{LยทmmHg}}{\text{molยทK}}

Choose R based on units of pressure and volume!

Standard Temperature and Pressure (STP)

Definition:

  • Temperature: 0ยฐC = 273.15 K
  • Pressure: 1 atm = 101.3 kPa = 760 mmHg = 760 torr

At STP, one mole of any ideal gas occupies:

V=22.4ย LV = 22.4 \text{ L}

This is a useful conversion factor!

Using PV = nRT

The ideal gas law connects all four variables

If you know any 3, you can find the 4th:

Example problems:

  1. Know P, V, T โ†’ find n (moles)
  2. Know n, T, P โ†’ find V (volume)
  3. Know n, V, P โ†’ find T (temperature)
  4. Know n, V, T โ†’ find P (pressure)

Key conversions:

  • Temperature: ยฐC + 273.15 = K
  • Pressure: 1 atm = 760 mmHg = 101.3 kPa
  • Volume: Usually given in L (if not, convert!)

Gas Density and Molar Mass

Density of a gas can be related to molar mass

Starting with PV = nRT:

n=mMn = \frac{m}{M}

Where:

  • mm = mass (g)
  • MM = molar mass (g/mol)

Substitute into ideal gas law:

PV=mMRTPV = \frac{m}{M}RT

Rearrange for density:

mV=PMRT\frac{m}{V} = \frac{PM}{RT}

d=PMRTd = \frac{PM}{RT}

Key relationships:

  • Higher molar mass โ†’ Higher density (at same T and P)
  • Higher temperature โ†’ Lower density (at same P and M)
  • Higher pressure โ†’ Higher density (at same T and M)

Why this is useful:

  • Calculate molar mass from density measurements
  • Predict relative densities of different gases
  • Explain why hot air rises (lower density)

Combined Gas Law

When amount of gas (n) is constant:

P1V1T1=P2V2T2\frac{P_1V_1}{T_1} = \frac{P_2V_2}{T_2}

This combines:

  • Boyle's Law: P1V1=P2V2P_1V_1 = P_2V_2 (constant T and n)
  • Charles's Law: V1T1=V2T2\frac{V_1}{T_1} = \frac{V_2}{T_2} (constant P and n)
  • Gay-Lussac's Law: P1T1=P2T2\frac{P_1}{T_1} = \frac{P_2}{T_2} (constant V and n)

Use when:

  • Gas undergoes change in conditions
  • Amount of gas stays the same
  • Need to find final state from initial state

Special cases:

Constant temperature (isothermal):

P1V1=P2V2P_1V_1 = P_2V_2 (Boyle's Law)

Constant pressure (isobaric):

V1T1=V2T2\frac{V_1}{T_1} = \frac{V_2}{T_2} (Charles's Law)

Constant volume (isochoric):

P1T1=P2T2\frac{P_1}{T_1} = \frac{P_2}{T_2} (Gay-Lussac's Law)

Dalton's Law of Partial Pressures

In a mixture of gases, each gas exerts pressure independently

Total pressure = Sum of partial pressures:

Ptotal=P1+P2+P3+...P_{total} = P_1 + P_2 + P_3 + ...

For each gas in the mixture:

Pi=ฯ‡iโ‹…PtotalP_i = \chi_i \cdot P_{total}

Where:

  • PiP_i = partial pressure of gas i
  • ฯ‡i\chi_i = mole fraction of gas i
  • PtotalP_{total} = total pressure

Mole fraction:

ฯ‡i=nintotal\chi_i = \frac{n_i}{n_{total}}

Key concept: Each gas behaves as if it alone occupies the entire volume

Application: Collecting Gas Over Water

Common lab technique:

  • Gas produced in reaction bubbles through water
  • Collected gas is mixture of desired gas + water vapor

Pressure relationship:

Ptotal=Pgas+PH2OP_{total} = P_{gas} + P_{H_2O}

Where:

  • PtotalP_{total} = atmospheric pressure
  • PgasP_{gas} = partial pressure of collected gas
  • PH2OP_{H_2O} = vapor pressure of water (depends on temperature)

To find amount of dry gas:

Pgas=Ptotalโˆ’PH2OP_{gas} = P_{total} - P_{H_2O}

Then use ideal gas law with PgasP_{gas}:

ngas=PgasVRTn_{gas} = \frac{P_{gas}V}{RT}

Water vapor pressure at common temperatures:

| Temp (ยฐC) | P(Hโ‚‚O) mmHg | |-----------|-------------| | 20 | 17.5 | | 25 | 23.8 | | 30 | 31.8 | | 35 | 42.2 |

Kinetic Molecular Theory (KMT)

Model explaining ideal gas behavior

Five Postulates

1. Gas particles are in constant, random motion

  • Particles move in straight lines until collision
  • Collisions are perfectly elastic (no energy lost)

2. Gas particles have negligible volume

  • Volume of particles << volume of container
  • Most of gas volume is empty space

3. No attractive or repulsive forces between particles

  • Particles don't interact except during collisions
  • Move independently

4. Average kinetic energy proportional to absolute temperature

KEavg=32RTKE_{avg} = \frac{3}{2}RT

Or for a single molecule:

KE=12mv2=32kBTKE = \frac{1}{2}mv^2 = \frac{3}{2}k_BT

Where:

  • mm = mass of particle
  • vv = velocity
  • kBk_B = Boltzmann constant = R/NAR/N_A

Higher temperature โ†’ Higher average KE โ†’ Faster particles

5. Collisions are perfectly elastic

  • Total kinetic energy conserved
  • Energy transferred between particles
  • No energy lost to heat, sound, etc.

Implications of KMT

Temperature and KE:

  • At same T, all gases have same average KE
  • Lighter gases move faster (same KE, less mass)

Root-mean-square speed:

vrms=3RTMv_{rms} = \sqrt{\frac{3RT}{M}}

Where:

  • RR = 8.314 J/(molยทK)
  • TT = temperature (K)
  • MM = molar mass (kg/mol)

Relationships:

  • vrmsโˆTv_{rms} \propto \sqrt{T} (higher T โ†’ faster)
  • vrmsโˆ1Mv_{rms} \propto \frac{1}{\sqrt{M}} (lighter โ†’ faster)

At same temperature:

  • He atoms move faster than Oโ‚‚ molecules
  • All have same average KE

Maxwell-Boltzmann Distribution

Not all particles have same speed!

Distribution of molecular speeds:

  • Some particles very slow
  • Most particles near average
  • Some particles very fast
  • Shape depends on temperature and molar mass

Effects of temperature:

  • Higher T โ†’ distribution shifts right (faster average)
  • Higher T โ†’ distribution broadens (wider range)
  • Peak becomes lower and flatter

Effects of molar mass:

  • Lower M โ†’ distribution shifts right (faster)
  • Lower M โ†’ distribution broadens

Effusion and Diffusion

Graham's Law of Effusion

Effusion: Gas escapes through tiny hole into vacuum

Rate of effusion inversely proportional to square root of molar mass:

rate1rate2=M2M1\frac{\text{rate}_1}{\text{rate}_2} = \sqrt{\frac{M_2}{M_1}}

Lighter gases effuse faster

Example: He effuses faster than Nโ‚‚

rateHerateN2=284=7โ‰ˆ2.65\frac{\text{rate}_{He}}{\text{rate}_{N_2}} = \sqrt{\frac{28}{4}} = \sqrt{7} \approx 2.65

Helium effuses 2.65 times faster than nitrogen

Diffusion

Diffusion: Gas spreads through space or through another gas

Also follows Graham's Law (approximately):

  • Lighter gases diffuse faster
  • Same mathematical relationship

Example: Smell of perfume spreading across room

Why faster with lighter gases?

  • Lighter โ†’ higher average velocity (from KMT)
  • Higher velocity โ†’ spreads faster

Real Gases vs. Ideal Gases

When Do Real Gases Deviate from Ideal Behavior?

Ideal gas law assumes:

  1. No volume (particles are points)
  2. No intermolecular forces

Real gases deviate when:

1. High pressure

  • Gas particles forced close together
  • Volume of particles becomes significant
  • Vreal>VidealV_{real} > V_{ideal}

2. Low temperature

  • Particles move slowly
  • IMFs have more effect
  • Particles attracted to each other
  • Preal<PidealP_{real} < P_{ideal}

General rule:

Real gases behave most ideally at:

  • Low pressure (particles far apart)
  • High temperature (high KE overcomes IMFs)

Real gases deviate most at:

  • High pressure (particles close)
  • Low temperature (IMFs significant)

Van der Waals Equation

Correction to ideal gas law for real gases:

(P+an2V2)(Vโˆ’nb)=nRT\left(P + \frac{an^2}{V^2}\right)(V - nb) = nRT

Pressure correction: an2V2\frac{an^2}{V^2}

  • Accounts for attractive forces
  • Reduces effective pressure
  • aa = strength of IMFs (larger for polar molecules)

Volume correction: nbnb

  • Accounts for volume of particles
  • Reduces available volume
  • bb = size of particles (larger for bigger molecules)

Constants a and b:

  • Specific to each gas
  • Larger a โ†’ stronger IMFs
  • Larger b โ†’ larger molecules

When van der Waals โ‰ˆ Ideal:

  • Low pressure (correction terms become small)
  • High temperature (KE >> IMFs)

Gas Stoichiometry

Using ideal gas law in chemical reactions

Mole Relationships

For reactions involving gases:

\ceaA(g)+bB(g)โˆ’>cC(g)+dD(g)\ce{aA(g) + bB(g) -> cC(g) + dD(g)}

Mole ratios from balanced equation:

  • At same T and P, volume ratios = mole ratios
  • This is Avogadro's Law

Example:

\ce2H2(g)+O2(g)โˆ’>2H2O(g)\ce{2H2(g) + O2(g) -> 2H2O(g)}

At same T and P:

  • 2 volumes Hโ‚‚ + 1 volume Oโ‚‚ โ†’ 2 volumes Hโ‚‚O
  • 2 moles Hโ‚‚ + 1 mole Oโ‚‚ โ†’ 2 moles Hโ‚‚O

Problem-Solving Strategy

Given: Conditions of gas (P, V, T) and reaction

Steps:

  1. Use PV = nRT to find moles of given gas
  2. Use stoichiometry (mole ratios) to find moles of desired gas
  3. Use PV = nRT to find conditions of desired gas

Or use directly:

P1V1n1T1=P2V2n2T2\frac{P_1V_1}{n_1T_1} = \frac{P_2V_2}{n_2T_2}

With n1n2\frac{n_1}{n_2} from stoichiometry

Summary of Gas Laws

| Law | Equation | Constant | Relationship | |-----|----------|----------|--------------| | Boyle's | P1V1=P2V2P_1V_1 = P_2V_2 | T, n | Inverse (Pโ†‘Vโ†“) | | Charles's | V1T1=V2T2\frac{V_1}{T_1} = \frac{V_2}{T_2} | P, n | Direct (Tโ†‘Vโ†‘) | | Gay-Lussac's | P1T1=P2T2\frac{P_1}{T_1} = \frac{P_2}{T_2} | V, n | Direct (Tโ†‘Pโ†‘) | | Avogadro's | V1n1=V2n2\frac{V_1}{n_1} = \frac{V_2}{n_2} | P, T | Direct (nโ†‘Vโ†‘) | | Combined | P1V1T1=P2V2T2\frac{P_1V_1}{T_1} = \frac{P_2V_2}{T_2} | n | - | | Ideal | PV=nRTPV = nRT | - | All variables | | Dalton's | PT=P1+P2+...P_T = P_1 + P_2 + ... | - | Partial pressures | | Graham's | r1r2=M2M1\frac{r_1}{r_2} = \sqrt{\frac{M_2}{M_1}} | - | Effusion rate |

Key Problem-Solving Tips

Always convert:

  • Temperature to Kelvin (K = ยฐC + 273.15)
  • Pressure to match R (usually atm)
  • Volume to match R (usually L)

Choose correct R:

  • Match units to pressure and volume
  • Most common: 0.0821 Lยทatm/(molยทK)

Partial pressures:

  • Use mole fractions
  • Account for water vapor when collecting gas

Real vs ideal:

  • Real gases โ†’ use at low P, high T
  • Deviations at high P, low T

Gas stoiometry:

  • Convert to moles first
  • Use mole ratios
  • Convert back to gas conditions

๐Ÿ“š Practice Problems

1Problem 1medium

โ“ Question:

A sample of nitrogen gas occupies 5.00 L at 25ยฐC and 1.50 atm. (a) How many moles of Nโ‚‚ are present? (b) What is the mass of the nitrogen gas? (c) If the temperature is increased to 100ยฐC at constant pressure, what will be the new volume?

๐Ÿ’ก Show Solution

Solution:

Given: V = 5.00 L, T = 25ยฐC = 298 K, P = 1.50 atm, R = 0.08206 Lยทatm/(molยทK)

(a) Moles using PV = nRT: n = PV/(RT) = (1.50 atm)(5.00 L) / [(0.08206)(298 K)] n = 7.50 / 24.45 = 0.307 mol Nโ‚‚

(b) Mass: Molar mass of Nโ‚‚ = 2(14.01) = 28.02 g/mol Mass = 0.307 mol ร— 28.02 g/mol = 8.60 g

(c) New volume (Charles's Law at constant P): Vโ‚/Tโ‚ = Vโ‚‚/Tโ‚‚ Tโ‚‚ = 100ยฐC = 373 K Vโ‚‚ = Vโ‚(Tโ‚‚/Tโ‚) = 5.00 L ร— (373 K / 298 K) Vโ‚‚ = 6.25 L

2Problem 2easy

โ“ Question:

A sample of nitrogen gas occupies 5.00 L at 25ยฐC and 1.50 atm. How many moles of nitrogen are present?

๐Ÿ’ก Show Solution

Solution:

Given:

  • Volume (V) = 5.00 L
  • Temperature (T) = 25ยฐC
  • Pressure (P) = 1.50 atm

Find: Number of moles (n)

Step 1: Convert temperature to Kelvin

T(K)=T(ยฐC)+273.15T(K) = T(ยฐC) + 273.15

T=25+273.15=298.15ย KT = 25 + 273.15 = 298.15 \text{ K}

Can round to 298 K for calculations

Step 2: Identify the appropriate gas constant

Units we have:

  • P in atm โœ“
  • V in L โœ“
  • T in K โœ“

Use: R=0.0821L\cdotpatmmol\cdotpKR = 0.0821 \frac{\text{Lยทatm}}{\text{molยทK}}

Step 3: Apply ideal gas law

PV=nRTPV = nRT

Solve for n:

n=PVRTn = \frac{PV}{RT}

Step 4: Substitute values

n=(1.50ย atm)(5.00ย L)(0.0821L\cdotpatmmol\cdotpK)(298ย K)n = \frac{(1.50 \text{ atm})(5.00 \text{ L})}{(0.0821 \frac{\text{Lยทatm}}{\text{molยทK}})(298 \text{ K})}

n=7.5024.5n = \frac{7.50}{24.5}

n=0.306ย moln = 0.306 \text{ mol}

Answer:

n=0.306ย molย N2\boxed{n = 0.306 \text{ mol N}_2}

Or: 0.31ย mol\boxed{0.31 \text{ mol}} (2 sig figs)

Check reasonableness:

At STP (1 atm, 273 K):

  • 1 mole occupies 22.4 L
  • Our conditions: Higher P (1.50 atm) and higher T (298 K)

Higher P โ†’ compressed โ†’ less volume per mole Higher T โ†’ expanded โ†’ more volume per mole

Net effect: Roughly 0.3 mol in 5 L seems reasonable

Alternative check using proportions:

At STP: 1 mol in 22.4 L

Our gas: 5.00ย L22.4ย L/molโ‰ˆ0.22\frac{5.00 \text{ L}}{22.4 \text{ L/mol}} \approx 0.22 mol at STP

But P is 1.5ร— higher โ†’ compress โ†’ more moles fit And T is ~1.09ร— higher โ†’ expand โ†’ fewer moles fit

Net: 0.22ร—1.5/1.09โ‰ˆ0.300.22 \times 1.5 / 1.09 \approx 0.30 mol โœ“

Units check:

atmโ‹…LL\cdotpatmmol\cdotpKโ‹…K=atmโ‹…Lโ‹…mol\cdotpKL\cdotpatmโ‹…K=mol\frac{\text{atm} \cdot \text{L}}{\frac{\text{Lยทatm}}{\text{molยทK}} \cdot \text{K}} = \frac{\text{atm} \cdot \text{L} \cdot \text{molยทK}}{\text{Lยทatm} \cdot \text{K}} = \text{mol} โœ“

Key concepts:

  1. Always convert temperature to Kelvin
  2. Match R units to given units
  3. Use PV = nRT when relating P, V, T, and n
  4. Check reasonableness against STP values

3Problem 3medium

โ“ Question:

A sample of nitrogen gas occupies 5.00 L at 25ยฐC and 1.50 atm. (a) How many moles of Nโ‚‚ are present? (b) What is the mass of the nitrogen gas? (c) If the temperature is increased to 100ยฐC at constant pressure, what will be the new volume?

๐Ÿ’ก Show Solution

Solution:

Given: V = 5.00 L, T = 25ยฐC = 298 K, P = 1.50 atm, R = 0.08206 Lยทatm/(molยทK)

(a) Moles using PV = nRT: n = PV/(RT) = (1.50 atm)(5.00 L) / [(0.08206)(298 K)] n = 7.50 / 24.45 = 0.307 mol Nโ‚‚

(b) Mass: Molar mass of Nโ‚‚ = 2(14.01) = 28.02 g/mol Mass = 0.307 mol ร— 28.02 g/mol = 8.60 g

(c) New volume (Charles's Law at constant P): Vโ‚/Tโ‚ = Vโ‚‚/Tโ‚‚ Tโ‚‚ = 100ยฐC = 373 K Vโ‚‚ = Vโ‚(Tโ‚‚/Tโ‚) = 5.00 L ร— (373 K / 298 K) Vโ‚‚ = 6.25 L

4Problem 4hard

โ“ Question:

A mixture of gases contains 0.500 mol Nโ‚‚, 0.300 mol Oโ‚‚, and 0.200 mol COโ‚‚ in a 10.0 L container at 27ยฐC. (a) Calculate the total pressure. (b) Calculate the partial pressure of each gas. (c) What is the mole fraction of oxygen?

๐Ÿ’ก Show Solution

Solution:

Given: n_Nโ‚‚ = 0.500 mol, n_Oโ‚‚ = 0.300 mol, n_COโ‚‚ = 0.200 mol V = 10.0 L, T = 27ยฐC = 300 K, R = 0.08206 Lยทatm/(molยทK)

(a) Total pressure (Dalton's Law): n_total = 0.500 + 0.300 + 0.200 = 1.00 mol

P_total = n_total RT/V = (1.00)(0.08206)(300) / 10.0 P_total = 2.46 atm

(b) Partial pressures: Using P_i = (n_i/n_total) ร— P_total or P_i = n_i RT/V

P_Nโ‚‚ = (0.500/1.00) ร— 2.46 = 1.23 atm P_Oโ‚‚ = (0.300/1.00) ร— 2.46 = 0.738 atm P_COโ‚‚ = (0.200/1.00) ร— 2.46 = 0.492 atm

Check: 1.23 + 0.738 + 0.492 = 2.46 atm โœ“

(c) Mole fraction of oxygen: ฯ‡_Oโ‚‚ = n_Oโ‚‚ / n_total = 0.300 / 1.00 = 0.300

Note: ฯ‡_Oโ‚‚ = P_Oโ‚‚ / P_total = 0.738 / 2.46 = 0.300 โœ“

5Problem 5hard

โ“ Question:

A mixture of gases contains 0.500 mol Nโ‚‚, 0.300 mol Oโ‚‚, and 0.200 mol COโ‚‚ in a 10.0 L container at 27ยฐC. (a) Calculate the total pressure. (b) Calculate the partial pressure of each gas. (c) What is the mole fraction of oxygen?

๐Ÿ’ก Show Solution

Solution:

Given: n_Nโ‚‚ = 0.500 mol, n_Oโ‚‚ = 0.300 mol, n_COโ‚‚ = 0.200 mol V = 10.0 L, T = 27ยฐC = 300 K, R = 0.08206 Lยทatm/(molยทK)

(a) Total pressure (Dalton's Law): n_total = 0.500 + 0.300 + 0.200 = 1.00 mol

P_total = n_total RT/V = (1.00)(0.08206)(300) / 10.0 P_total = 2.46 atm

(b) Partial pressures: Using P_i = (n_i/n_total) ร— P_total or P_i = n_i RT/V

P_Nโ‚‚ = (0.500/1.00) ร— 2.46 = 1.23 atm P_Oโ‚‚ = (0.300/1.00) ร— 2.46 = 0.738 atm P_COโ‚‚ = (0.200/1.00) ร— 2.46 = 0.492 atm

Check: 1.23 + 0.738 + 0.492 = 2.46 atm โœ“

(c) Mole fraction of oxygen: ฯ‡_Oโ‚‚ = n_Oโ‚‚ / n_total = 0.300 / 1.00 = 0.300

Note: ฯ‡_Oโ‚‚ = P_Oโ‚‚ / P_total = 0.738 / 2.46 = 0.300 โœ“

6Problem 6medium

โ“ Question:

A mixture of gases contains 2.00 mol He, 3.00 mol Ne, and 5.00 mol Ar at a total pressure of 800 mmHg. Calculate: (a) the mole fraction of each gas, (b) the partial pressure of each gas.

๐Ÿ’ก Show Solution

Solution:

Given:

  • nHen_{He} = 2.00 mol
  • nNen_{Ne} = 3.00 mol
  • nArn_{Ar} = 5.00 mol
  • PtotalP_{total} = 800 mmHg

Find: (a) Mole fractions, (b) Partial pressures


Part (a): Calculate mole fractions

Step 1: Find total moles

ntotal=nHe+nNe+nArn_{total} = n_{He} + n_{Ne} + n_{Ar}

ntotal=2.00+3.00+5.00=10.00ย moln_{total} = 2.00 + 3.00 + 5.00 = 10.00 \text{ mol}

Step 2: Calculate mole fraction of each gas

Mole fraction formula:

ฯ‡i=nintotal\chi_i = \frac{n_i}{n_{total}}

For helium:

ฯ‡He=2.00ย mol10.00ย mol=0.200\chi_{He} = \frac{2.00 \text{ mol}}{10.00 \text{ mol}} = 0.200

For neon:

ฯ‡Ne=3.00ย mol10.00ย mol=0.300\chi_{Ne} = \frac{3.00 \text{ mol}}{10.00 \text{ mol}} = 0.300

For argon:

ฯ‡Ar=5.00ย mol10.00ย mol=0.500\chi_{Ar} = \frac{5.00 \text{ mol}}{10.00 \text{ mol}} = 0.500

Check: Sum of mole fractions should equal 1

ฯ‡He+ฯ‡Ne+ฯ‡Ar=0.200+0.300+0.500=1.000\chi_{He} + \chi_{Ne} + \chi_{Ar} = 0.200 + 0.300 + 0.500 = 1.000 โœ“

Answer (a):

ฯ‡He=0.200,ฯ‡Ne=0.300,ฯ‡Ar=0.500\boxed{\chi_{He} = 0.200, \quad \chi_{Ne} = 0.300, \quad \chi_{Ar} = 0.500}


Part (b): Calculate partial pressures

Step 3: Use Dalton's Law of Partial Pressures

Relationship between mole fraction and partial pressure:

Pi=ฯ‡iโ‹…PtotalP_i = \chi_i \cdot P_{total}

For helium:

PHe=ฯ‡Heโ‹…PtotalP_{He} = \chi_{He} \cdot P_{total}

PHe=(0.200)(800ย mmHg)P_{He} = (0.200)(800 \text{ mmHg})

PHe=160ย mmHgP_{He} = 160 \text{ mmHg}

For neon:

PNe=ฯ‡Neโ‹…PtotalP_{Ne} = \chi_{Ne} \cdot P_{total}

PNe=(0.300)(800ย mmHg)P_{Ne} = (0.300)(800 \text{ mmHg})

PNe=240ย mmHgP_{Ne} = 240 \text{ mmHg}

For argon:

PAr=ฯ‡Arโ‹…PtotalP_{Ar} = \chi_{Ar} \cdot P_{total}

PAr=(0.500)(800ย mmHg)P_{Ar} = (0.500)(800 \text{ mmHg})

PAr=400ย mmHgP_{Ar} = 400 \text{ mmHg}

Check: Sum of partial pressures should equal total pressure

Ptotal=PHe+PNe+PArP_{total} = P_{He} + P_{Ne} + P_{Ar}

Ptotal=160+240+400=800ย mmHgP_{total} = 160 + 240 + 400 = 800 \text{ mmHg} โœ“

Answer (b):

PHe=160ย mmHg,PNe=240ย mmHg,PAr=400ย mmHg\boxed{P_{He} = 160 \text{ mmHg}, \quad P_{Ne} = 240 \text{ mmHg}, \quad P_{Ar} = 400 \text{ mmHg}}


Summary Table:

| Gas | Moles | Mole Fraction | Partial Pressure | |-----|-------|---------------|------------------| | He | 2.00 mol | 0.200 (20%) | 160 mmHg | | Ne | 3.00 mol | 0.300 (30%) | 240 mmHg | | Ar | 5.00 mol | 0.500 (50%) | 400 mmHg | | Total | 10.00 mol | 1.000 | 800 mmHg |

Key insights:

  1. Mole fraction = fraction of total moles

    • Dimensionless (no units)
    • Always between 0 and 1
    • Sum = 1.000
  2. Partial pressure proportional to mole fraction

    • Gas with most moles โ†’ highest partial pressure
    • Ar has 50% of moles โ†’ 50% of pressure
  3. Each gas behaves independently (Dalton's Law)

    • He exerts 160 mmHg as if alone in container
    • Ne exerts 240 mmHg as if alone in container
    • Ar exerts 400 mmHg as if alone in container
    • Total = sum of all partial pressures

Conceptual understanding:

Why does this work?

From ideal gas law for each gas:

Pi=niRTVP_i = \frac{n_iRT}{V}

Total pressure:

Ptotal=ntotalRTVP_{total} = \frac{n_{total}RT}{V}

Ratio:

PiPtotal=nintotal=ฯ‡i\frac{P_i}{P_{total}} = \frac{n_i}{n_{total}} = \chi_i

Therefore: Pi=ฯ‡iโ‹…PtotalP_i = \chi_i \cdot P_{total}

This is Dalton's Law!

7Problem 7hard

โ“ Question:

Hydrogen gas is collected over water at 25ยฐC and 745 mmHg atmospheric pressure. The volume of gas collected is 250.0 mL. The vapor pressure of water at 25ยฐC is 23.8 mmHg. (a) What is the partial pressure of the dry hydrogen gas? (b) How many moles of Hโ‚‚ were collected? (c) What mass of Hโ‚‚ was collected?

๐Ÿ’ก Show Solution

Solution:

Given:

  • Temperature = 25ยฐC
  • Total pressure (atmospheric) = 745 mmHg
  • Volume collected = 250.0 mL
  • Vapor pressure of Hโ‚‚O at 25ยฐC = 23.8 mmHg

Find: (a) Partial pressure of Hโ‚‚, (b) Moles of Hโ‚‚, (c) Mass of Hโ‚‚


Part (a): Partial pressure of dry Hโ‚‚

Step 1: Understand the situation

Gas collected over water contains:

  • Hโ‚‚ gas (what we want)
  • Hโ‚‚O vapor (from evaporation)

Total pressure = sum of partial pressures (Dalton's Law):

Ptotal=PH2+PH2OP_{total} = P_{H_2} + P_{H_2O}

Step 2: Solve for partial pressure of Hโ‚‚

PH2=Ptotalโˆ’PH2OP_{H_2} = P_{total} - P_{H_2O}

PH2=745ย mmHgโˆ’23.8ย mmHgP_{H_2} = 745 \text{ mmHg} - 23.8 \text{ mmHg}

PH2=721.2ย mmHgP_{H_2} = 721.2 \text{ mmHg}

Answer (a):

PH2=721.2ย mmHg=721ย mmHg\boxed{P_{H_2} = 721.2 \text{ mmHg} = 721 \text{ mmHg}}

This is the pressure of the DRY hydrogen gas


Part (b): Moles of Hโ‚‚

Step 3: Convert units for ideal gas law

Temperature:

T=25ยฐC+273.15=298.15ย Kโ‰ˆ298ย KT = 25ยฐC + 273.15 = 298.15 \text{ K} \approx 298 \text{ K}

Pressure: Convert mmHg to atm

PH2=721.2ย mmHgร—1ย atm760ย mmHgP_{H_2} = 721.2 \text{ mmHg} \times \frac{1 \text{ atm}}{760 \text{ mmHg}}

PH2=0.9489ย atmP_{H_2} = 0.9489 \text{ atm}

Volume: Convert mL to L

V=250.0ย mLร—1ย L1000ย mL=0.2500ย LV = 250.0 \text{ mL} \times \frac{1 \text{ L}}{1000 \text{ mL}} = 0.2500 \text{ L}

Step 4: Apply ideal gas law

PV=nRTPV = nRT

n=PVRTn = \frac{PV}{RT}

Use: R=0.0821L\cdotpatmmol\cdotpKR = 0.0821 \frac{\text{Lยทatm}}{\text{molยทK}}

Step 5: Calculate moles

nH2=(0.9489ย atm)(0.2500ย L)(0.0821L\cdotpatmmol\cdotpK)(298ย K)n_{H_2} = \frac{(0.9489 \text{ atm})(0.2500 \text{ L})}{(0.0821 \frac{\text{Lยทatm}}{\text{molยทK}})(298 \text{ K})}

nH2=0.237224.46n_{H_2} = \frac{0.2372}{24.46}

nH2=0.00970ย moln_{H_2} = 0.00970 \text{ mol}

Answer (b):

nH2=0.00970ย mol=9.70ร—10โˆ’3ย mol\boxed{n_{H_2} = 0.00970 \text{ mol} = 9.70 \times 10^{-3} \text{ mol}}

Or: 0.0097ย mol\boxed{0.0097 \text{ mol}} (2 sig figs)


Part (c): Mass of Hโ‚‚

Step 6: Convert moles to mass

Molar mass of Hโ‚‚:

MH2=2ร—1.008=2.016ย g/molM_{H_2} = 2 \times 1.008 = 2.016 \text{ g/mol}

Mass formula:

m=nร—Mm = n \times M

mH2=(0.00970ย mol)(2.016ย g/mol)m_{H_2} = (0.00970 \text{ mol})(2.016 \text{ g/mol})

mH2=0.0196ย gm_{H_2} = 0.0196 \text{ g}

mH2=19.6ย mgm_{H_2} = 19.6 \text{ mg}

Answer (c):

mH2=0.0196ย g=19.6ย mg\boxed{m_{H_2} = 0.0196 \text{ g} = 19.6 \text{ mg}}

Or: 0.020ย g\boxed{0.020 \text{ g}} (2 sig figs)


Summary of Results:

| Quantity | Value | |----------|-------| | (a) Partial pressure Hโ‚‚ | 721 mmHg (0.949 atm) | | (b) Moles Hโ‚‚ | 0.00970 mol | | (c) Mass Hโ‚‚ | 0.0196 g (19.6 mg) |


Key Concepts and Explanations:

1. Why subtract water vapor pressure?

When collecting gas over water:

  • Water evaporates into collection container
  • Total pressure includes both Hโ‚‚ and Hโ‚‚O vapor
  • Must subtract P(Hโ‚‚O) to get P(dry gas)

Diagram of setup:

  • Gas bubbles through water
  • Collected in inverted tube over water
  • Total P = P(Hโ‚‚) + P(Hโ‚‚O vapor)

2. Water vapor pressure depends on temperature

| Temperature | P(Hโ‚‚O) | |-------------|--------| | 20ยฐC | 17.5 mmHg | | 25ยฐC | 23.8 mmHg | | 30ยฐC | 31.8 mmHg |

Higher temperature โ†’ more evaporation โ†’ higher vapor pressure

3. Why use P(Hโ‚‚) not P(total) in ideal gas law?

Ideal gas law for Hโ‚‚ only:

PH2V=nH2RTP_{H_2}V = n_{H_2}RT

If we used P(total):

  • Would calculate moles of (Hโ‚‚ + Hโ‚‚O)
  • Wrong answer!

Must use partial pressure of Hโ‚‚ alone

4. Common mistakes to avoid:

โŒ Using P(total) instead of P(Hโ‚‚) โŒ Forgetting to convert ยฐC to K โŒ Forgetting to convert mL to L โŒ Using wrong vapor pressure for temperature

5. Check reasonableness:

At STP: 1 mol Hโ‚‚ = 22.4 L

Our conditions: ~0.01 mol in 0.25 L

Expected: 0.01ย mol0.25ย L=0.04\frac{0.01 \text{ mol}}{0.25 \text{ L}} = 0.04 mol/L

At STP: 1ย mol22.4ย L=0.045\frac{1 \text{ mol}}{22.4 \text{ L}} = 0.045 mol/L

Close! โœ“ (Our P slightly lower, T slightly higher than STP)

Mass check:

  • 0.01 mol ร— 2 g/mol = 0.02 g
  • Our answer: 0.0196 g โœ“

Everything checks out!

Application: This is how chemists measure amount of gas produced in reactions (like Hโ‚‚ from metal + acid).