Gas Laws Flashcards

0
Q

Kinetic Theory of Gases

A

1) The molecules/atoms that make up a gas have virtually no volume compared to the volume that the gas occupies. (This volume is due to motion of the gas molecules)
2) This motion is constant & random. (direction & speed)
3) All collisions between molecules are perfectly elastic (no loss of motion to other forms of energy).

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1
Q

Gas Laws

A

Mathematical relationships that describe properties of gases.

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2
Q

Pressure (P)

A

Force #of collisions
–––––
Area surface area of container

collisions { # particles present

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3
Q

Atmospheric (Atm) Pressure

A

Collisions from atmospheric gases with the dish of Hg. (Measured by height of Hg)

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4
Q

Standard Pressure (sea level)

A

760 mmHg
29.92 inHg
1 Atm
101.3 kPa

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5
Q

Water Pressure

A

10m of water = 1 Atm

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6
Q

Boules Law (1662)

A

For a fixed mass of gas at constant temp, the pressure & volume of the gas varies indirectly.
P1V1 = P2V2

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7
Q

Charles’ Law (1787)

A

For a fixed mass of gas at constant pressure, the Kelvin temp & volume of the gas varies directly.
V1 V2
–– = ––
T1 T2

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8
Q

Amonton Guy-Lussac’s Law (1802)

A

For a fixed mass of gas at constant volume, the Kelvin temp & pressure very directly.
P1 P2
–– = ––
T1 T2

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9
Q

Maldenburg Spheres

A

The particles of the atm colliding w/ the sphere on the outside & very few collisions on the inside, so the atm pushes the sphere together.
At same pressure: easy to separate b/c the collisions inside = collisions outside.

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10
Q

The Combined Gas Law

  • Sealed Container
  • Kelvin Temp.
A

P1V1 P2V2
––––– = –––––
T1 T2

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11
Q

Dalton’s Law of Partial Pressure

A

The total pressure for a mixture of gases is the sum of the individual pressures at the same conditions (vol & temp).
Σ IndPressure = Σ TotalPressure

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12
Q

Gas over Water (Wet Gas)

A

PAtmOutside = PDryGas + PH2OVapor

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13
Q

Ideal Gas Law

A
PV=nRT
R is universal gas constant 
8.21Atm
8.31kPa
6.24mmHg
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14
Q

Graham’s Law of Diffusion

A
The movement of gases/liquid/ions (solute) from areas of high concentration toward areas of low concentration until there is a uniform concentration throughout.
-Driven by Random Molecular Motion
RateA     √M. Mass B
–––––  =  –––––––––––
RateB     √M. Mass A
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