Chapter 5 The Gas Laws. Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force.

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Presentation transcript:

Chapter 5 The Gas Laws

Pressure  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force.  Container has the area.  Measured with a barometer.  Force per unit area.  Gas molecules fill container.  Molecules move around and hit sides.  Collisions are the force.  Container has the area.  Measured with a barometer.

Barometer  The pressure of the atmosphere at sea level will hold a column of mercury 760 mm Hg.  1 atm = 760 mm Hg  The pressure of the atmosphere at sea level will hold a column of mercury 760 mm Hg.  1 atm = 760 mm Hg 1 atm Pressure 760 mm Hg Vacuum

Manometer Gas h  Column of mercury to measure pressure.  h is how much lower the pressure is than outside.

Manometer  h is how much higher the gas pressure is than the atmosphere. h Gas

Units of pressure  1 atmosphere = 760 mm Hg  1 mm Hg = 1 torr  1 atm = 101,235 Pascals = kPa  Can make conversion factors from these.  1 atmosphere = 760 mm Hg  1 mm Hg = 1 torr  1 atm = 101,235 Pascals = kPa  Can make conversion factors from these.

The Gas Laws  Boyle’s Law  Pressure and volume are inversely related at constant temperature.  PV= k  As one goes up, the other goes down.  P 1 V 1 = P 2 V 2  Boyle’s Law  Pressure and volume are inversely related at constant temperature.  PV= k  As one goes up, the other goes down.  P 1 V 1 = P 2 V 2

Charles’s Law  Volume of a gas varies directly with the absolute temperature at constant pressure.  V = kT (if T is in Kelvin)  V 1 = V 2 T 1 = T 2  Volume of a gas varies directly with the absolute temperature at constant pressure.  V = kT (if T is in Kelvin)  V 1 = V 2 T 1 = T 2

Avogadro's Law At constant temperature and pressure, the volume of gas is directly related to the number of moles.  V = k n (n is the number of moles)  V 1 = V 2 n 1 n 2 At constant temperature and pressure, the volume of gas is directly related to the number of moles.  V = k n (n is the number of moles)  V 1 = V 2 n 1 n 2

Gay- Lussac Law  At constant volume, pressure and absolute temperature are directly related.  P = k T  P 1 = P 2 T 1 = T 2  At constant volume, pressure and absolute temperature are directly related.  P = k T  P 1 = P 2 T 1 = T 2

Combined Gas Law  If the moles of gas remains constant, use this formula and cancel out the other things that don’t change.  P 1 V 1 = P 2 V 2. T 1 T 2  If the moles of gas remains constant, use this formula and cancel out the other things that don’t change.  P 1 V 1 = P 2 V 2. T 1 T 2

Ideal Gas Law  PV = nRT  V = L at 1 atm, 0ºC, n = 1 mole, what is R?  R is the ideal gas constant.  R = L atm/ mol K  Tells you about a gas is NOW.  The other laws tell you about a gas when it changes.  PV = nRT  V = L at 1 atm, 0ºC, n = 1 mole, what is R?  R is the ideal gas constant.  R = L atm/ mol K  Tells you about a gas is NOW.  The other laws tell you about a gas when it changes.

Ideal Gas Law  An equation of state.  Independent of how you end up where you are at. Does not depend on the path.  Given 3 you can determine the fourth.  An equation of state.  Independent of how you end up where you are at. Does not depend on the path.  Given 3 you can determine the fourth.

Ideal Gas Law  An ideal gas is a hypothetical substance  Think of it as a limit.  Gases only approach ideal behavior at low pressure (< 1 atm) and high temperature.  Use the laws anyway, unless told to do otherwise. They give good estimates.  An ideal gas is a hypothetical substance  Think of it as a limit.  Gases only approach ideal behavior at low pressure (< 1 atm) and high temperature.  Use the laws anyway, unless told to do otherwise. They give good estimates.

Gas Density and Molar Mass  D = m/V  Let M stand for molar mass  M = m/n  n= PV/RT  M = m PV/RT  M = mRT = m RT = DRT PV V P P  D = m/V  Let M stand for molar mass  M = m/n  n= PV/RT  M = m PV/RT  M = mRT = m RT = DRT PV V P P

Gases and Stoichiometry  Reactions happen in moles  At Standard Temperature and Pressure (STP, 0ºC and 1 atm) 1 mole of gas occuppies L.  If not at STP, use the ideal gas law to calculate moles of reactant or volume of product.  Reactions happen in moles  At Standard Temperature and Pressure (STP, 0ºC and 1 atm) 1 mole of gas occuppies L.  If not at STP, use the ideal gas law to calculate moles of reactant or volume of product.

Examples  Mercury can be achieved by the following reaction  What volume of oxygen gas can be produced from 4.10 g of mercury (II) oxide at STP?  At 400.ºC and 740 torr?  Mercury can be achieved by the following reaction  What volume of oxygen gas can be produced from 4.10 g of mercury (II) oxide at STP?  At 400.ºC and 740 torr?

Dalton’s Law  The total pressure in a container is the sum of the pressure each gas would exert if it were alone in the container.  The total pressure is the sum of the partial pressures.  P Total = P 1 + P 2 + P 3 + P 4 + P 5...  For each P = nRT/V  The total pressure in a container is the sum of the pressure each gas would exert if it were alone in the container.  The total pressure is the sum of the partial pressures.  P Total = P 1 + P 2 + P 3 + P 4 + P 5...  For each P = nRT/V

Dalton's Law  P Total = n 1 RT + n 2 RT + n 3 RT +... V V V  In the same container R, T and V are the same.  P Total = (n 1 + n 2 + n )RT V  P Total = (n Total )RT V  P Total = n 1 RT + n 2 RT + n 3 RT +... V V V  In the same container R, T and V are the same.  P Total = (n 1 + n 2 + n )RT V  P Total = (n Total )RT V

The mole fraction  Ratio of moles of the substance to the total moles.  symbol is Greek letter chi      = n 1 = P 1 n Total P Total  Ratio of moles of the substance to the total moles.  symbol is Greek letter chi      = n 1 = P 1 n Total P Total

Examples 3.50 L O L N atm  When these valves are opened, what is each partial pressure and the total pressure? 4.00 L CH atm atm

Vapor Pressure  Water evaporates!  When that water evaporates, the vapor has a pressure.  Gases are often collected over water so the vapor. pressure of water must be subtracted from the total pressure.  It must be given.  Water evaporates!  When that water evaporates, the vapor has a pressure.  Gases are often collected over water so the vapor. pressure of water must be subtracted from the total pressure.  It must be given.

Example  N 2 O can be produced by the following reaction  what volume of N 2 O collected over water at a total pressure of 94 kPa and 22ºC can be produced from 2.6 g of NH 4 NO 3 ? ( the vapor pressure of water at 22ºC is 21 torr)  N 2 O can be produced by the following reaction  what volume of N 2 O collected over water at a total pressure of 94 kPa and 22ºC can be produced from 2.6 g of NH 4 NO 3 ? ( the vapor pressure of water at 22ºC is 21 torr)

Kinetic Molecular Theory  Theory tells why the things happen.  explains why ideal gases behave the way they do.  Assumptions that simplify the theory, but don’t work in real gases.  The particles are so small we can ignore their volume.  The particles are in constant motion and their collisions cause pressure.  Theory tells why the things happen.  explains why ideal gases behave the way they do.  Assumptions that simplify the theory, but don’t work in real gases.  The particles are so small we can ignore their volume.  The particles are in constant motion and their collisions cause pressure.

Kinetic Molecular Theory  The particles do not affect each other, neither attracting or repelling.  The average kinetic energy is proportional to the Kelvin temperature.  Appendix 2 shows the derivation of the ideal gas law and the definition of temperature.  We need the formula KE = 1/2 mv 2  The particles do not affect each other, neither attracting or repelling.  The average kinetic energy is proportional to the Kelvin temperature.  Appendix 2 shows the derivation of the ideal gas law and the definition of temperature.  We need the formula KE = 1/2 mv 2

What it tells us  (KE) avg = 3/2 RT  This the meaning of temperature.  u is the particle velocity.  u is the average particle velocity.  u 2 is the average particle velocity squared.  the root mean square velocity is  u 2 = u rms  (KE) avg = 3/2 RT  This the meaning of temperature.  u is the particle velocity.  u is the average particle velocity.  u 2 is the average particle velocity squared.  the root mean square velocity is  u 2 = u rms

Combine these two equations  (KE) avg = N A (1/2 mu 2 )  (KE) avg = 3/2 RT  (KE) avg = N A (1/2 mu 2 )  (KE) avg = 3/2 RT

Combine these two equations  (KE) avg = N A (1/2 mu 2 )  (KE) avg = 3/2 RT Where M is the molar mass in kg/mole, and R has the units J/Kmol.  The velocity will be in m/s  (KE) avg = N A (1/2 mu 2 )  (KE) avg = 3/2 RT Where M is the molar mass in kg/mole, and R has the units J/Kmol.  The velocity will be in m/s

Range of velocities  The average distance a molecule travels before colliding with another is called the mean free path and is small (near )  Temperature is an average. There are molecules of many speeds in the average.  Shown on a graph called a velocity distribution  The average distance a molecule travels before colliding with another is called the mean free path and is small (near )  Temperature is an average. There are molecules of many speeds in the average.  Shown on a graph called a velocity distribution

number of particles Molecular Velocity 273 K

number of particles Molecular Velocity 273 K 1273 K

number of particles Molecular Velocity 273 K 1273 K

Velocity  Average increases as temperature increases.  Spread increases as temperature increases.  Average increases as temperature increases.  Spread increases as temperature increases.

Effusion  Passage of gas through a small hole, into a vacuum.  The effusion rate measures how fast this happens.  Graham’s Law the rate of effusion is inversely proportional to the square root of the mass of its particles.  Passage of gas through a small hole, into a vacuum.  The effusion rate measures how fast this happens.  Graham’s Law the rate of effusion is inversely proportional to the square root of the mass of its particles.

Effusion  Passage of gas through a small hole, into a vacuum.  The effusion rate measures how fast this happens.  Graham’s Law the rate of effusion is inversely proportional to the square root of the mass of its particles.  Passage of gas through a small hole, into a vacuum.  The effusion rate measures how fast this happens.  Graham’s Law the rate of effusion is inversely proportional to the square root of the mass of its particles.

Deriving  The rate of effusion should be proportional to u rms  Effusion Rate 1 = u rms 1 Effusion Rate 2 = u rms 2  The rate of effusion should be proportional to u rms  Effusion Rate 1 = u rms 1 Effusion Rate 2 = u rms 2

Diffusion  The spreading of a gas through a room.  Slow considering molecules move at 100’s of meters per second.  Collisions with other molecules slow down diffusions.  Best estimate is Graham’s Law.  The spreading of a gas through a room.  Slow considering molecules move at 100’s of meters per second.  Collisions with other molecules slow down diffusions.  Best estimate is Graham’s Law.

Examples  A compound effuses through a porous cylinder 3.20 time faster than helium. What is it’s molar mass?  If mol of NH 3 effuse through a hole in 2.47 min, how much HCl would effuse in the same time?  A sample of N 2 effuses through a hole in 38 seconds. what must be the molecular weight of gas that effuses in 55 seconds under identical conditions?  A compound effuses through a porous cylinder 3.20 time faster than helium. What is it’s molar mass?  If mol of NH 3 effuse through a hole in 2.47 min, how much HCl would effuse in the same time?  A sample of N 2 effuses through a hole in 38 seconds. what must be the molecular weight of gas that effuses in 55 seconds under identical conditions?

Diffusion  The spreading of a gas through a room.  Slow considering molecules move at 100’s of meters per second.  Collisions with other molecules slow down diffusions.  Best estimate is Graham’s Law.  The spreading of a gas through a room.  Slow considering molecules move at 100’s of meters per second.  Collisions with other molecules slow down diffusions.  Best estimate is Graham’s Law.

Real Gases  Real molecules do take up space and they do interact with each other (especially polar molecules).  Need to add correction factors to the ideal gas law to account for these.  Real molecules do take up space and they do interact with each other (especially polar molecules).  Need to add correction factors to the ideal gas law to account for these.

Volume Correction  The actual volume free to move in is less because of particle size.  More molecules will have more effect. Pressure Correction  Because the molecules are attracted to each other, the pressure on the container will be less than ideal  depends on the number of molecules per liter.  The actual volume free to move in is less because of particle size.  More molecules will have more effect. Pressure Correction  Because the molecules are attracted to each other, the pressure on the container will be less than ideal  depends on the number of molecules per liter.