2.4.3 · D1States of Matter (Quantitative)

Foundations — Dalton's law of partial pressures

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Before you can trust a single formula in the parent note, you must be able to read every letter in it. This page takes each symbol Dalton's law leans on — , , , , , , — and builds it from a picture. We go slowly. If you know all of these already, jump to the parent note; otherwise, read top to bottom.


1. What is a gas, as a picture?

Forget formulas for a moment. A gas is a huge number of tiny particles (molecules) flying in straight lines, occasionally bouncing off each other and off the container walls. They are mostly empty space between them.

Figure — Dalton's law of partial pressures

This is exactly the model of Kinetic Theory of Gases. We only need its cartoon here.


2. Pressure — "push per unit area"

When a ball hits a wall and bounces back, it shoves the wall a tiny bit. Millions of balls hitting every second add up to a steady push. Spread that push over the area of the wall, and you get pressure.

Figure — Dalton's law of partial pressures

Units you will meet:

  • atmosphere (atm) — roughly the air pressure at sea level.
  • millimetre of mercury (mmHg) — how tall a column of mercury the pressure can hold up; .

3. Volume — the size of the box

The picture: the box that holds the swarm. Two ideas about volume matter for Dalton's law:

  1. A gas fills its whole container — molecules spread out until they hit walls. There is no "unfilled corner."
  2. In a mixture, every gas occupies the same full volume . Red balls and blue balls share the whole box; neither is squeezed into a corner.

4. Temperature — how fast the balls fly

Kelvin, not Celsius — and why it must be kelvin.

Absolute zero () is where molecular motion stops entirely. Because appears as a multiplier in , doubling must double the push — but that only works from a scale that starts at "no motion at all." Celsius starts at the freezing point of water, which is arbitrary, so it would give nonsense (e.g. dividing by C).


5. Amount — counting molecules by the mole

You cannot count balls one by one, so chemists bundle them.

The picture: is just "how many balls" repackaged into convenient units. More moles = more balls = more bangs = more pressure (at fixed ).


6. The gas constant — the conversion glue

You don't derive ; you look it up. Its job is purely to balance units. The specific value is chosen so that pressure comes out in atm and volume in litres — the units used throughout the parent's examples.


7. The ideal gas equation — assembling the symbols

Now that , , , , each have a picture, the master equation reads like a sentence.

This is the Ideal Gas Equation. Every partial-pressure formula in the parent note is this equation applied to one gas at a time. That is why we built its five symbols first.


8. Partial pressure — the subscript that means "just this gas"

Lowercase (partial) versus uppercase (total) is a deliberate convention: small = one gas's share, big = everyone together.

Figure — Dalton's law of partial pressures

9. Mole fraction — "your share of the crowd"

Two facts you must feel, not just memorise:

  • is always between and (you can't have a negative share or more than everything).
  • The shares add to one: — everyone's slice together is the whole pie.

That second fact is why the partial pressures automatically sum back to the total: multiply "shares that add to 1" by and you recover . This is the machinery of Mole Fraction and Concentration Terms.


10. Aqueous tension — the one extra idea for "gas over water"

When a gas bubbles up through water, some water evaporates into it. That water vapour has its own partial pressure, called aqueous tension.

This is a special case of Vapour Pressure. You need it because the barometer over water reads gas + water vapour, and Dalton's law lets you subtract the water's share:


Prerequisite map

Gas as a swarm of balls

Pressure P push per area

Volume V size of box

Temperature T ball speed

Amount n moles counts balls

Gas constant R unit glue

Ideal gas law PV = nRT

Partial pressure pi one gas alone

Mole fraction xi your share

Dalton law Ptotal = sum pi

Aqueous tension gas over water


Equipment checklist

Cover the right side; if you can answer each, you are ready for the parent note.

What does pressure physically measure?
The total force from molecular collisions divided by the wall area — push per unit area.
Why must temperature be in kelvin for ?
Kelvin starts at absolute zero (no motion), so works as a true multiplier; Celsius's arbitrary zero would break the proportionality.
Convert C to kelvin.
.
What is a mole, and why count in moles instead of grams?
A fixed count of particles; pressure depends on the number of colliding molecules, not their mass.
What is the value and job of in ?
; it makes the units on both sides balance.
Difference between (capital) and (lowercase)?
is the total pressure of the whole mixture; is the pressure of gas alone in the same .
Define mole fraction and give its range.
, the share of molecules that are gas ; always between 0 and 1.
Why do all mole fractions add to 1?
Every molecule belongs to exactly one gas, so the shares partition the whole and must total the entire amount.
What is aqueous tension?
The saturated vapour pressure of water at a given temperature — water vapour's fixed partial-pressure contribution over water.
Compute the pressure of gas in at .
.

Connections

  • Ideal Gas Equation — the master equation these symbols assemble into.
  • Kinetic Theory of Gases — the swarm picture behind pressure and temperature.
  • Mole Fraction and Concentration Terms — the home of .
  • Vapour Pressure — background for aqueous tension.
  • Real Gases and van der Waals Equation — what changes when the "no interaction" cartoon fails.