Assignment 6 Flashcards
properties of a gas
volume
density
mass/amount/moles
pressure
IMFs (what do they determine)
determine physical properties
Particle Theory/Kinetic Molecular Theory
particles…
are meaured in moles (6.02 x 1023)
have mass
are the smallest representative unit of a substance that contain the properties of the larger substance
travel randomly in a straight line
speed indicate its heat
have no IMFs (ideal gas assumption)
collide with each other and the walls of the container (measured by vol and pressure)
particles
the smallest representative unit of a substance that contains the properties of the larger substance
ideal gas assumption
no IMFs
PV = nRT
theoretical
no freezing/boiling point
no energy (heat) lost
Relationship of Pressure to Volume
Inverse
same # particles + more volume/space = less bumping of particles = less pressure
same # particles + less volume/space = more bumping = more pressure
Relationship of Pressure to Temperature
Direct (if you start at absolute zero)
more temp = more movement of particles = more bumping = more pressure
less temp = less movement of particles = less bumping = less pressure
Relationship of Temperature to Volume
Direct (if you start at absolute zero)
more temp = more motion = more collision = more push on conainer = more volume
less temp = less motion = less collision = less push on conainer = less volume
Relationship of Number of Moles (n) to Pressure/Temperature/Volume
Direct
more moles = more mass = more vol
more moles = more particles in same space = more bumping = more pressure
more moles = more particles bumping = more KE/heat = more temp
Proportionality Constant R =
- 0821 (for atm)
- 314 (for kPa)
- 396 (for mmHg/torr)
what happens as a system is cooled
density increases
kinetic energy (temp) decreases
pressure decreases
volume decreases
particles squish together (IMFs became important, no ideal gas assumptions no equations)
solid
low KE
IMFs > KE of particles
incompressable
maintains shape and vol
liquid
medium KE
IMFs ≈ KE of particles
incompressable
constant vol, variable shape
gas
high KE
IMFs (essentially zero) < KE
compressable
no set vol or shape
boyle’s law
P1V1 = P2V2
charles’ law
V1/T1 = V2/T2
Gay-Lussac’s Law
P1/T1 = P2/T2
gas law equation for descriptive and changing moles
PV = nRT
gas law equation for changing conditions, constant moles
P1V1 P2V2
———— = nR = ———-
T1 T2
mole fraction equation
Px nx
—————— = —————–
PTOTAL nTOTAL