Chapter 6_Air Pressure
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Transcript of Chapter 6_Air Pressure
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AIR PRESSURE
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Keeping an Atmosphere
Atmosphere is keptby the worlds gravity
Low mass (small) worlds= low gravity
=almost no atm.
High mass (large) worlds = high gravity
= thick atm.
Gravity and pressure Air pressure depends on how much gas there
is i.e. The atmospheric thickness.
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Gravity and Atmospheric Pressure
The stronger the gravity, the more gas is held by the
world and the greater the weight of atm. on a point
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Earths Atmosphere
About 10 kmthick
Consists mostlyof molecularnitrogen (N2)
and oxygen (O2)
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The air is made up of molecules.
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Gravity pulls the air molecules
toward the earth, giving them
weight. The weight of the airmolecules all around us is
called the air pressure.
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High altitudes = lower pressure
Low altitudes = higher pressure
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Atmospheric Pressure
Gas pressuredepends on both
density and
temperature.
Adding airmolecules
increases the
pressure in a
balloon.
Heating the airalso increases
the pressure.
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Air pressure is
equal in all
directions.
Pressure = force per unit area
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As
elevation
goes up
Barometric
pressure
goes
down.
This is an inverse relationship.
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to
measure
airpressure.
A Barometer
is
used
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In 1643, Evangelista Torricelli
invented the barometer
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Torricellis barometer
used a glass column
suspended in a bowl of
mercury. The pressure
of the air molecules
pushed the mercury upinto the glass tube.
The weight of the mercury in
the tube was equal to the
weight of the air pressing
down on the mercury in the
dish.
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Asatmospheric
pressure
increases
The mercury in
the tube rises.
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The Mercury Barometer
Good: Bad:
Simple to construct
Highly accurate
Glass tube is fragile
Mercury is verytoxic!
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TheAneroidBarometer
No fragile tubes!
No toxic chemicals!
No batteries!Never needs winding!
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An aneroid barometer
uses a cell which has
had most of the airremoved.
As the air pressure
around the cell
increases, it presseson the cell, which
causes the needle to
move.
Television weather forecasters usually give barometric
pressure in inches of mercury. However, meteorologists
measure atmospheric pressure in millibars.
MILLIBARS
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Two types of barometric pressure measurements:
Station pressure is the actual
pressure at the recordinglocation. It is affected by the
local altitude.
Sea level pressure isreferenced to sea
level, so it has thesame altitude
anywhere in the
world.
Station pressure on a mountain top
will be lower than station pressure
in a valley. Scientists need a fixed
point of reference in order to
compare barometer readings in
different locations. That is why
barometer readings are sometimes
adjusted for elevation above sea
level at the station location.
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Most aneroid
barometers have a
needle which can be
set to remember the
previous reading.
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Changing Pressure
A rising barometer= increasing air pressure.
This usually means:
Rising barometer readings indicate that a
high pressure system is approaching.Higher atmospheric pressure is usually
associated with fair weather and clearing
skies.
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Changing Pressure
A falling barometer= decreasing air pressure.
This usually means:
Falling barometer readings usually
indicate the approach of an area of
low pressure. Low pressure readingsare usually associated with storm
systems. Tornadoes and hurricanes
can produce very low barometric
readings.
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Air Movement and Flow
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Fluids (air and water) flow from areas ofhigh pressure to areas of low pressure.
Change in pressure across a horizontaldistance is a pressure gradient.
Greater the difference in pressure and the shorter the
distance between them, the steeper the pressuregradient and the stronger the wind.
Movement of air across a pressure gradient
parallel to Earths surface is called a wind
and winds are named for the direction fromwhich they come.
6-1
Isobars in millibars the closer the isobar the
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Isobars in millibars, the closer the isobar thestronger the winds
High Pressure
Low Pressure
Rain
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The Atmosphere in Motion Atmospheric pressure is a measure of the force
pressing down on the Earths surface from the
overlying air. Pressure is often measured in different units including:
atmospheres (1 atmosphere is the average atmosphericpressure at sea level),
millibars (1 atmosphere = 1013.25 millibars), pounds per square inch or psi (1 atmosphere = 14.7 poundsper square inch),
mm or inches of mercury (1 atmosphere = 760 mm or 29.92inches of mercury)
torrs (1 torr = the pressure exerted by 1 cm of mercury). Low air density results in rising air and low surface
pressure. High air density results in descending air and high
surface pressure.
C
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Heating and Cooling of
Air
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The Gas Law Ideal Gas follows kinetic molecular theory, made up of large
number of molecules that are in rapid random motionfollowing perfect elastic collitions losing no momentum How the Kinetic Molecular Theory Explains the Gas Laws
The pressure of a gas results from collisions between the gasparticles and the walls of the container.
Each time a gas particle hits the wall, it exerts a force on thewall.
An increase in the number of gas particles in the containerincreases the frequency of collisions with the walls and thereforethe pressure of the gas.
Avogadro's Hypothesis As the number of gas particles increases, the frequency of
collisions with the walls of the container must increase. This, in turn, leads to an increase in the pressure of the gas. Flexible containers, such as a balloon, will expand until the
pressure of the gas inside the balloon once again balances thepressure of the gas outside.
Thus, the volume of the gas is proportional to the number of gasparticles.
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The Gas Laws Charles Law
The volume of a gas increased with the temperature The volume of a given amount of dry ideal gas is directly
proportional to the Kelvin Temperature provided the amountof gas and the pressure remain fixed.
When we plot the Volume of a gas against the Kelvin
temperature it forms a straight line. V1 / T1 = V2 / T2
Boyles Law the product of the pressure and volume are observed to be
nearly constant.
The product of pressure and volume is exactly a constant foran ideal gas.
p * V = constant
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WATER VAPOR
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(9.8oC)