Properties Of Gases (chpt. 10) Flashcards
Gas
A gas is any substance that has no well-defined boundaries but diffuses rapidly to fill any container in which it is placed
Three states of matter
Solid
Liquid
Gas
To convert from °C to K
Add 273
stp
Standard temperature and pressure
Standard temperature
273 Kelvin
0°C
Standard pressure
1 x 10^5 Pa
100 kPa
Boyles Law
States that, at constant temperature, the volume of a fixed mass of gas is inversely proportional to its pressure
pV = k
Charles Law
States that, at constant pressure, the volume of a fixed mass of gas is directly proportional to its temperature measured on the Kelvin scale
V
— = k
T
Combined gas law
By combining boyles law and Charles law
(stp)
P V. P V
——. =. ——
T. T
T = Kelvin
P = P
V = V
i.e if the volume is given in L use 22.4L at stp
Gay - Lussac’s Law of combining volumes
States that, in a reaction between gases, the volume of the reacting gases and the volume of any gaseous products are in the ratio of small whole numbers, provided the volumes are measured at the same temperature and pressure
Avogadros law
States that equal volumes of gases contain equal numbers of particles under the same conditions of temperature and pressure
At stp one mole of gas occupies 22.4 L
Assumptions of the kinetic theory
- Gases are made up of particles that are in CONTINUOUS, RAPID, RANDOM MOTION, colliding with each other and with the walls of the container
- There are NO attractive/repulsive forces between the particles of the gas
- The gas particles are so small and widely separated that the TOTAL VOLUME of all the particles is NEGLIGIBLE compared with the space they occupy
- Collisions between particles are PERFECTLY ELASTIC
- The average kinetic energy of the particles in a sample of gas is proportional to the temperature measured on the Kelvin scale
Limitations of the kinetic theory of gases
- There ARE forces of attraction/repulsion between the particles of a gas (van der Waals etc)
- The total volume of the particles of a gas is not negligible
Ideal gas
One that obeys all the assumptions of the kinetic theory of gases under all conditions of temperature and pressure