Chapters 10 and 12: Gases - PowerPoint PPT Presentation

1 / 23
About This Presentation
Title:

Chapters 10 and 12: Gases

Description:

Kinetic theory particles in all states of matter are in ... naphthalene (moth balls) 11. F. Adding/Removing Gas (Ch. 12): Review: Gases have a lot of K.E. ... – PowerPoint PPT presentation

Number of Views:20
Avg rating:3.0/5.0
Slides: 24
Provided by: Jar104
Category:
Tags: chapters | gases | moth

less

Transcript and Presenter's Notes

Title: Chapters 10 and 12: Gases


1
Chapters 10 and 12 Gases
  • A. Kinetic Theory (Ch. 10)
  • Kinetic energy (K.E.) the energy due to motion
  • Kinetic theory particles in all states of
    matter are in constant motion
  • - gas particles are spread out, move
    in straight paths, and fill up the shape of
    its container
  • - gas particles collide randomly with
    each other and are perfectly elastic
    (energy is completely transferred)

2
  • B. Gas Pressure (Ch. 10)
  • Gas pressure the pressure or force exerted by
    the collisions gas particles
  • Atmospheric pressure the pressure that results
    from collisions of air
    molecules with objects
  • - the higher the elevation
    (mountain vs. sea level), the lower
    the atmospheric pressure (thinner air)
  • Barometer measures atmospheric pressure

3
  • Units of pressure
  • 1 atm (atmosphere)
  • 101.3 kPa (kiloPascals)
  • 760 mmHg (millimeters of Mercury)
  • 760 torr (torr)
  • Convert using either proportions or factor-label
    method
  • STP (Standard Temperature and Pressure)
  • 0 ?C 273 K (temperature)
  • 1 atm or its equivalents (pressure)
  • Gases are temperature and pressure dependent

4
  • C. Kinetic energy and Kelvin temperature (Ch.
    10)
  • Kelvin temperature an adjusted scale from the
    Celsius temperature used for gases
    (see gas laws)
  • - no degree symbol used (K)
  • - formula K ?C 273
  • - Kelvin temp is directly
    proportional to K.E.
  • ex. At 200 K gas particles have 2x the K.E.
    compared to gas particles at 100 K
  • Absolute zero the temp when all particles stop
    moving (0 K -273 ?C -459 ?F)

5
  • Very cold temperatures vs. absolute zero
  • ex. Coldest temp. on earth (Antarctica)
  • 184 K -89 ?C -128 ?F
  • Liquid nitrogen
  • 77 K -196 ?C -321 ?F
  • Pluto
  • 40 K -233 ?C -387 ?F
  • Absolute zero
  • 0 K -273 ?C -459 ?F

6
  • D. Liquids ? Gases (Ch. 10)
  • Vapor pressure the pressure when a liquid
    starts to evaporate, and the gas
    particles in a sealed container collide
    with the container wall
  • - force of the gas above a liquid
    in a sealed container
  • - as temperature increases, so
    does the vapor pressure
  • - after time, the vapor (gas)
    starts to condense (liquid) until it
    reaches equilibrium (the rate of
    vaporization equals the rate of
    condensation)

7
  • Vapor pressure
  • ex.

8
  • Boiling point (B.P.) the temperature at which
    the vapor pressure is equal to the
    external pressure (atmospheric pressure)
  • Normal boiling point the B.P. at 1 atm (or its
    equivalents) of pressure
  • ex.

9
  • Graph of vapor pressure vs. temperature
  • ex.

10
  • E. Solids ? Gases (Ch. 10)
  • Sublimation when a solid goes straight into
    vapor (gas) without becoming a liquid
  • - these solids have very high vapor
    pressures (volatile)
  • ex. dry ice (CO2(s) ? CO2(g))
  • ice cubes after time in the freezer
  • freeze-dried foods
  • air fresheners
  • naphthalene (moth balls)

11
  • F. Adding/Removing Gas (Ch. 12)
  • Review
  • Gases have a lot of K.E.
  • Gases fill their container
  • Empty/open space between gas particles
  • Gases are compressible (squeezed together)
  • Variables that affect gases
  • P (pressure)
  • V (volume)
  • T (temperature, in Kelvin)
  • n (moles)

12
  • Adding gas to a sealed container
  • Increases the number of collisions
  • More collisions, greater pressure
  • Too much pressure, container breaks
  • If you add 2x the gas, the pressure doubles
  • Removing gas from a sealed container
  • Pressure decreases
  • Gas goes from a high-pressure sealed container to
    a low-pressure surroundings
  • Gases prefer to be at low pressure so there is
    more room for the particles to move around and
    collide with one another

13
  • G. Boyles Law (Ch. 12)
  • Boyles law pressure vs. volume at a constant
    temperature (same temperature)
    with no gas being added/removed
  • - formula P1 x V1 P2 x V2
  • - both Ps and Vs need to be in the
    same units
  • - inverse relationship (P ?, V ?)
  • ex.

14
  • ex. A balloon contains 30.0 L of He(g) at 101.3
    kPa. What is the volume when the balloon has a
    new pressure of 0.5 atm?
  • P1 x V1 P2 x V2
  • (1 atm) x (30.0 L) (0.5 atm) x V2
  • 0.5 atm 0.5 atm
  • V2 60 L

15
  • H. Charless Law (Ch. 12)
  • Charless law temperature vs. volume at a
    constant pressure (same pressure) with no
    gas being added/removed
  • - formula V1 V2
  • T1 T2
  • - both Ts must be in Kelvin
  • - both Vs must be the same unit
  • - direct relationship (T ?, V ?)
  • ex.

16
  • Why Kelvin temperature?

17
  • ex. A balloon at 24 ?C has a volume of 4 L. The
    balloon is heated to 58 ?C. What is the new
    volume of the balloon?
  • V1 V2
  • T1 T2
  • (4 L) x (331 K) (297 K) x V2
  • 297 K 297 K
  • V2 4.46 L

18
  • I. Gay-Lussacs Law (Ch. 12)
  • Gay-Lussacs law temperature vs. pressure at a
    constant volume (same volume)
    with no gas being added/removed
  • - formula P1 P2
  • T1 T2
  • - both Ts must be in Kelvin
  • - both Ps must be the same unit
  • - direct relationship (T ?, P ?)
  • ex.

19
  • J. Combined Gas Law (Ch. 12)
  • Combined gas law combines all 3 main gas laws
  • - formula P1 x V1 P2 x V2
  • T1 T2
  • - cross out the variable (if any)
    that remains constant or not
    mentioned in the problem
  • - both Ts must be in Kelvin
  • - both Ps and Vs must have the
    same units
  • - STP 0 ?C (273 K) and 1 atm

20
  • ex. A filled balloon has a volume of 30 L at 40
    ?C and 153 kPa. What will the volume of the
    balloon be at STP?
  • P1 153 kPa P2 101.3 kPa
  • V1 30 L V2 ?
  • T1 313 K T2 273 K
  • V2 (V1 x P1 x T2) / (P2 x T1)
  • V2 (30 L x 153 kPa x 273 K) / (101.3 kPa x
    313 K)
  • V2 39.5 L

21
  • K. Ideal Gas Law (Ch. 12)
  • Ideal gases the way all gases should behave in
    a perfect world
  • Real gases the way gases behave in the real
    world
  • Ideal gas law describes the behavior of ideal
    gas
  • formula P V n R T
  • P (atm)
  • V (L) at STP 22.4 L
  • n (moles)
  • T (K)
  • Gas law constant (R) 0.0821 (L?atm)/(moles?K)
  • (will be given on test/quiz)

22
  • ex. A 20.0 L container is filled with gas to
    obtain a pressure of 202.6 kPa at 28 ?C. How
    many moles of N2(g) are in the container?
  • P V n R T
  • n (P V) / (R T)
  • n (2 atm) x (20.0 L)
  • (0.0821 L?atm/moles?K) x (301 K)
  • n 1.62 moles

23
  • L. Daltons Law of Partial Pressures (Ch. 12)
  • Daltons law the sum of the partial pressures
    of each gas in a mixture is equal to
    the total pressure at a constant
    temperature at volume
  • - formula PT P1 P2 P3
  • ex. What is the partial pressure of O2 at STP if
    the other partial pressures of air are
  • N2 79.10 kPa CO2 0.04 kPa Ar 0.94
    kPa
  • 101.3 kPa 79.1 kPa 0.04 kPa 0.94 kPa
    PO2
  • 101.3 kPa 80.08 kPa PO2
  • PO2 21.22 kPa
Write a Comment
User Comments (0)
About PowerShow.com