Gasses

download Gasses

of 18

description

gases

Transcript of Gasses

  • 16 6 GasesGasesPrepared by

    Dr Mohd Zul Helmi Rozaini

    University of East Anglia

    University Malaysia Terengganu

    6.1 The states of matter6.1 The states of matter

    Matter exists in only three states: _________ _________ _________

    The most stable state of a particular substance can be changed by __________________________

    6.2 Describing gases6.2 Describing gases

    Gases ________________________ ____________________ This implies that the individual gas

    atoms or molecules are free to move anywhere within their container

    Therefore the forces between them ____________________

    6.2 Describing gases6.2 Describing gases

    The defining characteristic of gases is the pressure they exert

    The pressure (p) exerted by a gas is dependent on: ______________ ______________ ______________

  • 26.2 Describing gases6.2 Describing gases

    Pressure (p) At any temperature above absolute zero,

    atoms/molecules are always in motion

    Pressure is the collective result of these collisions

    6.2 Describing gases6.2 Describing gases

    The atmosphere exerts pressure on the Earths surface

    The pressure of the

    A measures the difference in pressures exerted by

    6.2 Describing gases6.2 Describing gases 6.2 Describing gases6.2 Describing gases

    The SI unit for pressure is pascal (Pa) 1 Pa = 1 N m-2

    A number of non-SI units are used:

  • 3 The gas laws -The atoms

    The volume occupied by a gas changes in response to changes in pressure, temperature and amount of gas

    6.2 Describing gases6.2 Describing gases

    Law Boyle investigated gases in a J-shaped tube

    Determined

    6.2 Describing gases6.2 Describing gases

    Law Determined the volume of

    a gas is directly proportional to its

    Law Gas volume is directly

    proportional to the amount

    6.2 Describing gases6.2 Describing gases 6.2 Describing gases6.2 Describing gases

    The ideal gas equation All four variables (p, V, T and n) can be

    related using a single constant This is known as the gas constant (R) In SI units, R = 8.314 J mol-1 K-1

    pV = This is known as

  • 4WE6.1: Calculation of gas pressureWE6.1: Calculation of gas pressure

    A 1.00 x 103 L steel storage tank contains 88.5 kg of methane, CH4. If the temperature is 25C, what is the pressure of the inside tank?

    WE6.2: PressureWE6.2: Pressure-- volume variationsvolume variations

    A sample of helium gas is held at constant temperature inside a cylinder with a volume of 0.80 L when a piston exerts a pressure of 1.5 x 105 Pa. if the external pressure on the piston is increased to 2.1 x 105, what will the new volume be?

    6.3 Molecular view of gases6.3 Molecular view of gases

    As gases are

    molecules,the most important energy component to consider is their kinetic energy, Ekinetic

    The kinetic energy of an object is given by the equation:

    Molecular speeds A molecular beam

    apparatus measures the speeds of molecules in a gas

    6.3 Molecular view of gases6.3 Molecular view of gases

  • 5 Speed and energy The energy of a molecule is related to its

    speed At a given temperature, all

    6.3 Molecular view of gases6.3 Molecular view of gases

    Average kinetic energy The most probable kinetic energy is not

    the same as the average kinetic energy The average kinetic energy of gas

    molecules depends on the temperature of the gas

    6.3 Molecular view of gases6.3 Molecular view of gases

    6.4: Molecular kinetic energy6.4: Molecular kinetic energy

    Determine the average molecular kinetic energy and molar kinetic energy of gaseous sulfur hexafluoride, SF6, at 150C

    6.3 Molecular view of gases6.3 Molecular view of gases

    Ideal gases An ideal gas has the following two

    characteristics: The volume occupied by the molecules of an

    ideal gas is negligible compared with the volume of its container.

    The energies generated by forces among ideal gas

  • 66.3 Molecular view of gases6.3 Molecular view of gases

    How does an gas behave? Consider how changes in V, T or n affect the

    pressure, p In an ideal gas each molecule is

    independent of all others

    Lets consider the effect of changing one property while holding the other properties constant

    Increasing the amount of gas: Pressure is directly proportional to the

    amount of gas This

    6.3 Molecular view of gases6.3 Molecular view of gases

    Changing the : Pressure is inversely proportional to volume This agrees

    6.3 Molecular view of gases6.3 Molecular view of gases Changing :

    Pressure is directly proportional to temperature

    This is in agreement with

    6.3 view of gases6.3 view of gases

  • 76.4 Additional gas properties6.4 Additional gas properties

    Determination of molar mass The ideal gas equation can be combined

    with n = m/M to find the molar mass of an unknown gas

    pV = nRT can be used

    This information can then be used

    6.4 Additional gas properties6.4 Additional gas properties

    Gas The density of a gas varies significantly

    with the conditions The ideal gas equation and n = m/M can

    be combined and rearranged to obtain an :

    WE6.5: Molar mass determinationWE6.5: Molar mass determination

    Calcium carbide, CaC2 is a hard, grey-black solid with melting point of 2000C. It reacts vigorously with water to produce a gas and a solution containing OH- ions.

    A 12.8 g sample of CaC2 was treated with excess water and resulting gas was collected in an evacuated 5.00 L glass bulb with a mass of 1254.49 g. the filled bulb had a mass of 1259.70 and the pressure of the gas inside was 1.00 x 105Pa when the temperature was 26.8C.

    Calculate the molar mass of the gas and determine its formula. (Assume that the product gas is insoluble in water, and the vapor pressure of water is neglible in relation to the pressure of the product gas)

    6.4 Additional gas properties6.4 Additional gas properties

    The equation reveals three features of gas density: The density of an ideal gas increases linearly

    with pressure at fixed temperature

    The density of an ideal gas increases linearly with molar mass at a given temperature and pressure

    Gas density has a significant effect on interactions

  • 8WE6.6: Gas densityWE6.6: Gas density

    A hot air balloon will rise when the density of its air is 15% lower than that of the atmospheric air. Calculate the density of air at 298 K and 1.0 x 105 Pa (assume that dry air is 78% N2and 22% O2), and determine the minimum temperature of air that will cause a balloon to rise

    6.4 Additional gas properties6.4 Additional gas properties

    Rates The temperature of a gas determines

    the average speed of the gas molecules of which it is comprised To state this dependence quantitatively:

    This is called the root-mean-square speed

    6.4 Additional gas properties6.4 Additional gas properties

    Effusion The movement of molecules

    6.4 Additional gas properties6.4 Additional gas properties

  • 9 Diffusion The movement of one type of molecule

    6.4 Additional gas properties6.4 Additional gas properties 6.5 Gas mixtures6.5 Gas mixtures

    Gas behaviour depends on the number of gas atoms or molecules but not on their identity

    Daltons law of partial pressures In a mixture of gases in which no chemical

    reaction occurs, each gas

    6.5 Gas mixtures6.5 Gas mixtures

    Describing gas mixtures Mole fraction (X)

    The number of moles of a substance as a fraction of the number of moles of all substances in the mixture

    The partial pressure of a component in a gas mixture is its mole fraction

    6.5 Gas mixtures6.5 Gas mixtures

  • 10

    6.5 Gas mixtures6.5 Gas mixtures

    When referring to lower concentrations in a gas mixture, scientists use parts per million (ppm) or parts per billion (ppb)

    Mole fractions is moles per mole ppm is moles per million moles ppb is moles per billion moles 1 ppm is a mole fraction of

    WE6.7: Gas mixtureWE6.7: Gas mixture

    Exactly 8.00 g of O2 and 2.00 g of He place in a 5.00 L tank at 298 K. Determine the total pressure of the mixture, and find the partial pressures and mole fractions of the two gases

    WE6.8: Working with (WE6.8: Working with (ppmppm))

    The exhaust gas from an average car contains 206 ppm of the pollutant nitrogen oxide, NO. If a car emits 0.125 m3 of exhaust gas at 1.00 x 105Pa and exactly 350 K, what mass of NO has been added to the atmosphere?

    6.6 Gas stoichiometry6.6 Gas stoichiometry

    The principles of stoichiometry apply equally to solids, liquids and gases

    No matter what phase substances are in, their chemical behaviour can be described in molecular terms

    For gases,

  • 11

    WE6.9: Gas WE6.9: Gas stoichiometrystoichiometry WE6.5 described the synthesis of ethyne, C2H2, from calcium

    carbide, CaC2. Modern industrial production of ethyne is based on a reaction of methane, CH4, under carefully controlled conditions. At temperature greater than 1600 K, two methane molecules rearrange to give three molecules of hydrogen and one molecule of ethyne

    2CH4 (g) C2H2 (g)+ 3H2 (g)

    A 50.0 L steel vessel, filled with CH4 to a pressure of 10.0x105 Pa at 298 K, is heated to exactly 1600 K to convert CH4 into C2H2. What is the maximum possible mass of C2H2that can be produced?What pressure does the reactor reach at 1600 K? Assume that both CH4 and C2H2 behave as ideal gases under the conditions of the reaction.

    WE6.10: limiting WE6.10: limiting ragentsragents in a in a gas mixturegas mixture

    Margarine cn be made from natural oils such as coconut oil by hydrogenation.

    C57H104O6 (l) + 3H2 (g) -> C57H110O6 (s) An industrial hydrogenator with a volume of

    2.50 x 102 L is charged with 12.0 kg of oil and 7.00 x 105 Pa of hydrogen,H2 at 473 K. The reaction produces the maximum amount of margarine. What is the final pressure of H2 and what mass of margarine will be produced? Assume that H2 behaves as ideal gas under the reaction condition.

    6.6 Gas stoichiometry6.6 Gas stoichiometry 6.7 Intermolecular forces6.7 Intermolecular forces

    The halogens Exist as diatomic

    molecules Although they have similar

    covalent bonding, bromine and

  • 12

    When the average kinetic energy is large enough, molecules remain separated from and the substance is a gas

    When intermolecular

    6.7 Intermolecular forces6.7 Intermolecular forces 6.7 Intermolecular forces6.7 Intermolecular forces

    Real gases The ideal gas model makes two

    assumptions:

    Neither of these assumptions is true for a real gas

    How close do real gases come to ideal behaviour?

    6.7 Intermolecular forces6.7 Intermolecular forces

    The ideal gas model can still be used to discuss the properties of real gases, as long as conditions do not become too extreme

    6.7 Intermolecular forces6.7 Intermolecular forces

  • 13

    The van der Waals equation A modified ideal gas equation that accounts

    for attractive forces and molecular volumes

    Adds two

    Each correction term includes a constant that has a specific value for every gas

    6.7 Intermolecular forces6.7 Intermolecular forces 6.7 Intermolecular forces6.7 Intermolecular forces

    WE6.12:Van WE6.12:Van derder WaalsWaals Gasses such as methane are sold and

    shipped in compresses gas cylinders. A typical cylinder has a volume of 15.0 L and when full, contains 62.0 mol of CH4. after prolonged use, 0.620 mol of CH4 remains in the cylinder.

    Use the Van der Waals equation to calculate the pressures in the cylinder when full and after use, and compare the values to those obtained from the ideal gas equation. Assume a constant temperature of 27C

    6.7 Intermolecular forces6.7 Intermolecular forces

    Melting and boiling points Can be used as indicators of the

    strengths of intermolecular forces The boiling point is the temperature at

    which the average kinetic energy of molecular motion balances the attractive energy of intermolecular attractions

    When the pressure is 1.013 x 105 Pa, that temperature is the normal boiling point

  • 14

    6.7 Intermolecular forces6.7 Intermolecular forces

    The conversion of a liquid into a gas is called vaporisation

    Condensation is the reverse process At temperatures below the freezing point,

    the molecules become locked in place and the liquid solidifies. When the pressure is , that temperature is the normal freezing point

    Boiling

    6.7 Intermolecular forces6.7 Intermolecular forces

    6.8 Types of intermolecular 6.8 Types of intermolecular forcesforces

    There are three general types: Dispersion forces

    The attractions between the negatively charged electron clouds and the positively charged nuclei of neighbouring molecules

    6.8 Types of intermolecular 6.8 Types of intermolecular forcesforces

    Dispersion forces Exists because the electron clouds of

    molecules can be distorted

    Dispersion forces are the net attractive forces between

  • 15

    The magnitude of dispersion forces depends on how easy it is to distort the electron cloud of a molecule

    This ease

    6.8 Types of intermolecular 6.8 Types of intermolecular forcesforces

    Dispersion forces increase in strength with the number or electrons

    6.8 Types of intermolecular 6.8 Types of intermolecular forcesforces

    For molecules with comparable numbers of electrons, the shape of the molecule makes an

    6.8 Types of intermolecular 6.8 Types of intermolecular forcesforces

    Dipolar forces

    6.8 Types of intermolecular 6.8 Types of intermolecular forcesforces

  • 16

    6.8 Types of intermolecular 6.8 Types of intermolecular forcesforces

    Hydrogen bonds There are two requirements:

    First, there must be an electron-deficient hydrogen atom that can be attracted to an electron pair

    Hydrogen atoms in O-H, F-H and N-H bonds meet this requirement

    6.8 Types of intermolecular 6.8 Types of intermolecular forcesforces

    6.8 Types of intermolecular 6.8 Types of intermolecular forcesforces

    Hydrogen bonds can form between different molecules

    Molecules can form more than one hydrogen bond (eg glycine)

    Hydrogen bonds can form within a molecule (eg salicylic acid)

    Hydrogen bonding is particularly important in biochemical systems

    Binary hydrogen compounds It is both the strength and number of

    hydrogen bonds that a binary hydrogen compound can form which determines its boiling point

    6.8 Types of intermolecular 6.8 Types of intermolecular forcesforces

  • 17

    SummarySummary

    The three most important states of matter are solid, liquid and gas

    Gases occupy all of the space in which they are contained

    The pressure exerted by a gas is due to the collisions of rapidly moving gas atoms or molecules with the walls of the container

    SummarySummary

    Boyles Law, Charles Law and Avogadros Law describe the relationships between volume and pressure, volume and temperature, and volume and amount of a gas respectively

    The combination of these laws gives the ideal gas equation, pV = nRT

    SummarySummary

    In order to determine the kinetic energy of a gas molecule, it is necessary to measure the speed with which it is moving

    All gases have an identical molecular kinetic energy distribution

    Real gases approximate ideal behaviour under certain conditions

    SummarySummary

    The movement of gas molecules can be described as either effusion or diffusion

    Each gaseous component in a mixture of ideal gases exerts a partial pressure

    The mole fraction of a substance equals the ratio of moles to the total number of moles

  • 18

    SummarySummary

    Intermolecular forces are partially responsible for the fact that real gases do not exactly obey the ideal gas laws

    The van der Waals equation for a real gas makes corrections for the volume of the gas molecules and for the attractive force between them

    Melting and boiling points give good indications of the strength of intermolecular forces

    SummarySummary

    There are three general types of intermolecular forces: Dispersion forces Dipolar forces Hydrogen bonds