force exerted when gas molecules strike the area of a container wall
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vacuum
opposite of pressure; a deficit of molecules
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SI Pressure unit
Pascals (Pa); 1 Pa = 1N/m^2
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1 barr =
10^5 Pa
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1 atm =
101.325 kPa, 760 torr, 760 mmHg, 14 lb/in^2
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barometer
-an instrument that measures atmospheric pressure -the pressure at the bottom of the Hg tube is balanced by atmospheric pressure on the dish -h is proportional to P
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Most common pressure units
torr and atm
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Hydrostatic pressure
pressure exerted by a fluid due to gravity
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hydrostatic pressure equation
p=rho(h)(g)
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wind
created by air moving from high to low pressure
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manometer
-measures gas trapped in a container -delta h is proportional to pressure
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Why do hot air balloons rise?
-due to buoyant force -hot air is less dense than normal air (less gas mlx) -causes balloon to rise
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the atmosphere
exerts a large pressure on objects on earth's surface
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Atmospheric pressure analogy
like a bowling ball on a thumbnail
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exosphere
>700 km
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thermosphere
80-700 km
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mesosphere
50-80 km
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stratosphere
12-50 km
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troposphere
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Air density and temperature in troposphere
increase with distance from the earth
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Other units
ppm, ppb, and ppt
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Selenium
protects the body against an excess of heavy metals
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Where does the jet stream exist?
stratosphere
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state function
-depends on initial and final volume -path independent -denoted by a capital letter
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Collisions of an ideal gas
must be completely elastic
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ideal gas
hypothetical construct that real gases approximate under certain conditions
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ideal gas law
-relates P, V, n, T -most gases are ideal at room temp -accurate for low P and moderate T
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first hot air balloon
caught on fire due to use of hydrogen gas
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Luer
end of syringe with a specific length and taper
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Absolute zero
zero kelvin, -273.15 C
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Celsius and Kelvin intervals
are equal
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Charles' Law
-volume is proportional to temperature -P and n are held constant -V1/T1 = V2/T2
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Charles' Law origin
extrapolates so P=0 @ T=-273 C
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Charles' Law Graph (V and T)
linear
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Boyle's Law
-volume varies inversely with pressure -T and n are constant -P1V1 = P2V2
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Graph of P vs. V
parabolic
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Graph of 1/P vs. V
linear
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What prevents containers from collapsing?
collisions from gas molecules inside the container counteract the atmospheric pressure
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STP
T=273.15 K P=1 atm
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standard molar volume
22.4 L
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Gay-Lussac's Law
-pressure and temperature are proportional -V and n are constant -P1/T1 = P2/T2
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Gay-Lussac's Law graph (P and T)
linear
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Gay-Lussac's law synonym
Amontons' Law
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Ideal Gas Law
PV=nRT
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Combined Gas Law
PV/nT = R = PV/nT
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Antoine Lavoisier
-father of modern chemistry -made quantitative strides by studying gases
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Gas density
d=MP/RT
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Molar Mass Equation
M=m/n
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Pressure in a Mixture of Gases
-individual gases do not affect each other's pressures -each gas exerts the same pressure it would alone
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Partial Pressure
pressure exerted by an individual gas in a mixture
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Dalton's Law of Partial Pressures
Pt = Pa + Pb + Pc...
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Mole Fraction (X)
-unit of concentration -# of moles of component/ total # of moles
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Mole Fraction equation
Pa = Xa(Pt) when Xa = na/nt
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Collection of Gases over Water
-bottle is inverted in water dish -reaction runs that produces a gas -gas bubbles into bottle -gas pressure = atmospheric pressure when the water level is equal in and out of the bottle
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saturation of gas with vapor
Ptotal = Pgas + Pvapor
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Vapor Pressure of Water
pressure exerted by water vapor in equilibrium with liquid water in closed container; depends on temperature
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boiling point
the point where gas and liquid phase are in equilibrium
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Mixing of Ideal gases
ideal gases are completely miscible and form homogeneous mixtures
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lighter gas particles....
move faster
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Mean Free Path
average distance a molecule travels between collisions; increases with decreasing V
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Diffusion
-molecule put in closed container disperse quickly -results in a equal concentration of gases
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Rate of Diffusion
amount of gas passing thru area/unit of time
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Effusion
escape of gas molecules through a tiny hole
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Graham's Law of effusion
the rate of effusion is inversely proportional to molar mass
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Graham's Law equation
ratea/rateb = SQrt(Mb)/SQrt(Ma)
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compression
increases temperature
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expansion
decreases temperature
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pressure of chemical reactions in the lab
constant
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maxwell-boltzmann distribution
distribution curve broadens with higher average
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V total in ideal gas =
Vspace + Vparticles(0)
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molecular velocity is proportional to
molecular mass
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compression of liquids and solids
extremely difficult
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Kinetic Molecular Theory
a simple microscopic model that effectively explains the gas laws
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First Article of KMT
a gas consists of tiny molecules in random, rapid motion; molecules change direction after collision
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Second Article of KMT
Gas molecules are small compared to the distances between them, making them compressible and miscible
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Third Article of KMT
Gas molecules exert pressure thru collisions between molecules and molecule walls
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Fourth Article of KMT
Gas molecules has small attraction/repulsion for each other
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Fifth Article of KMT
Gas molecules make elastic collisions with each other and do not lose energy thru collision
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Kinetic Energy depends on
temperature and n
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kinetic energy and temperature
directly proportional
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Peak on Maxwell Curve
most probable particle speed
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Vrms on maxwell curve
after the peak when the graph switches from increasing to decreasing
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Speed distribution flattens...
as temperature increases
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Vrms
square root of average squares of speed where n= number of particles
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Average KE =
1/2 Mvrms
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KMT and Amonton's Law
-KE increases with T -more collisions = higher P
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KMT and Boyle's Law
-V decreases, decreasing wall area -more frequent collision = higher P
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KMT and Avogadro's Law
-V increase = n increase -more mlxs require greater space to reduce collision and keep P constant
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KMT and Dalton's Law
-gas molecules of one gas bombard walls regardless of other gases -Ptotal = total bombardment from all gases
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KMT and effusion
effusion depends on the average speed of molecules
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Vrms a / Vrms b
SqrtMb/SqrtMa
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low Pressure deviation
negative
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high Pressure deviation
positive
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Compressibility Factor (Z)
actual volume of one mole of gas divided by molar volume of an ideal gas at the same temperature and pressure
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When Z=1
the gas is ideal
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Gases at High pressure
-molecules begin to crowd and volume of the molecules becomes appreciable -attractive force becomes more signficant