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Thermodynamics Chapter 3 Thermodynamics Chapter 3

Thermodynamics Chapter 3 - PowerPoint Presentation

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Thermodynamics Chapter 3 - PPT Presentation

Daily Temperature Variations Diurnal temperature range the difference between the daily maximum and minimum temperature 2 Daily Temperature Variations Factors that control how warm it can get during the day include ID: 929973

decreases temperature air pressure temperature decreases pressure air lapse parcel dry rate heat atmosphere increases exercise process potential stays

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Slide1

Thermodynamics

Chapter 3

Slide2

Daily Temperature Variations

Diurnal temperature range = the difference between the daily maximum and minimum temperature.2

Slide3

Daily Temperature Variations

Factors that control how warm it can get during the day include:Season – warmer in summer than winterPresence of clouds or haze will reduce warmingType of soil and soil moisture content –

less warming with moist soil

Presence or absence of vegetation

more warming without vegetation

Snow cover

will reduce temperature

3

Slide4

Daily Temperature Variations

Coldest nighttime temperatures and strongest nocturnal inversions occur with:Winter – long night and long period of radiative coolingClear skies – allows LW radiative loss from ground with little downwelling LW from the atmosphere

Light winds

reduce depth of atmosphere that cools by turbulent heat fluxes so this thin layer can become very cold

Snow cover

insulates the atmosphere from warmer ground below and is an effective emitter of LW radiation

4

Slide5

The Earth’s Annual Energy Budget

On an annual basis, the earth and atmosphere have a balance between energy gained and lost.5

Each part of the atmosphere (top, atmosphere, and ground) must be in energy balance.

Slide6

Regional Temperature Variations

Factors controlling temperature variability across Earth:Latitude – T decreases with increasing latitudeLand/water distribution

larger temperature variation over continents than over oceans

Ocean currents

warm currents like Gulf Stream or cold currents like along the west coast of North America

Elevation

T decreases with elevation (removed from figures)

6

Average January Temperature (

)

 

Average July Temperature (

)

 

Slide7

Regional Temperature Variations

Temperature gradient is larger between the tropics and the pole in the winter hemisphere.The warmest air occurs in the sub-tropics of the summer hemisphere (NH in July, SH in January).The main reason ocean temperatures varies less than continental temperatures is that water has a larger heat capacity than land so oceans warm and cool less than land for the same radiative input.Ocean currents transport heat to reduce the amount of warming and cooling locally.

7

Slide8

Apparent Temperature Indices

How hot or cold we feel depends on more than just the air temperature.The human body transfers energy from/to its environment by:Radiation – LW loss by humans and LW & SW gain from environment

Conduction and turbulent transfer

Evaporation

latent heat

The wind chill and heat indices attempt to account for how exposed skin “feels” under windy or humid conditions compared to reference conditions.

8

Slide9

Apparent Temperature Indices

Wind Chill IndexTemperature and wind impact how cold we feelWater on the skin will evaporate and cool a personFrostbite = freezing of the skinHypothermia = a lowering of the body’s core temperature below its normal range

9

Slide10

Apparent Temperature Indices

The heat index accounts for the role of humidity in making you feel warmer (or cooler) than the actual air temperature.In the summer, high humidity limits how much sweat can evaporate and thus limits how effectively the human body can cool itself.

10

Slide11

Review + Exercices

11

Slide12

Lapse Rate (

Process (parcel) lapse rate = the lapse rate of an air parcel experiencing a specific process (such as moving vertically through the atmosphere):

Theoretical lapse rate

C

an be determined using the First

L

aw of

T

hermo

!

Environmental lapse rate = the lapse rate of the air surrounding an air parcel:

Observational lapse rate

Can be determined by launching a radiosonde!

12

Slide13

Exercise 1

Calculate the environmental lapse of the troposphere for the standard atmosphere temperature profile shown here.

 

11 km

-56.5

 

1

5

 

13

Slide14

Exercise 1

Troposphere:At z1 = 0 km, T

1

= 15

At z

2

= 11 km, T

2

= -56.5

 

 

→ T decreases 6.5 K for every 1 km increase in altitude in the troposphere.

11 km

-56.5

 

1

5

 

14

 

 

 

Slide15

Dry Adiabatic Lapse Rate (

)

 

DALR = an air parcel lapse rate when no heat (energy) enters or leaves the air parcel (

).

 

 

DALR is larger than the average lapse rate in the troposphere (

) calculated before.

The standard atmosphere is not completely dry (contains water).

Water has a high heat capacity, which acts to decrease the lapse rate.

 

15

Slide16

Exercise 2

Suppose you hike down in the Grand Canyon on a dry day (

). On the rim, the temperature is 95

(35

). In the canyon, 1500m below, how hot is it?

 

 

Don’t forget to convert T in K!!

16

Slide17

Exercise 2

What do we know?

What

are

we

looking

for?

 

 

 

 

 

 

17

Slide18

Potential Temperature (

)

 

The potential temperature can be calculated using:

Potential temperature will not change as the parcel rises or sinks for a dry adiabatic process because no heat is added or removed from the air parcel.

Potential temperature is conserved (constant) for a dry adiabatic process but the temperature of the air parcel will change.

 

Always use SI units!! (temperature in K and pressure in Pa)

Poisson’s Equation

18

Slide19

Exercise 3

What is the potential temperature

at NCAR’s Mesa Lab? (you can assume dry air)

 

19

Slide20

Exercise 3

1st method:

2

nd

method:

 

20

Need to know T and z!

Need to know T and p!

Slide21

Exercise 4

If a parcel is lifted dry adiabatically, what happens to pressure, temperature, and potential temperature q?

Pressure increases, temperature decreases,

q

increases

Pressure increases, temperature increases,

q

decreases

Pressure decreases, temperature stays the same,

q

decreases

Pressure decreases, temperature decreases,

q

stays the same

Pressure decreases, temperature increases,

q

stays the same

21

Slide22

Exercise 4

If a parcel is lifted dry adiabatically, what happens to pressure, temperature, and potential temperature q?Pressure increases, temperature decreases,

q

increases

Pressure increases, temperature increases,

q

decreases

Pressure decreases, temperature stays the same,

q

decreases

Pressure decreases, temperature decreases,

q

stays the same

Pressure decreases, temperature increases,

q

stays the same

22

Slide23

Thermodynamic Diagram

Pressure

Temperature

isobars = lines

of constant pressure

isotherms = lines of

constant temperature

dry

adiabats

= lines of constant potential temperature

23

Slide24

Thermodynamic Diagram

Dry adiabats:

Relate temperature and pressure at different levels in the atmosphere for a dry adiabatic process on a thermodynamic diagram.

Represent the process lapse rate for a dry adiabatic process (a process in which no heat is exchanged with the parcel and no phase change of water occur).

24

Slide25

Exercise 5

25

Air parcel:

p = 750

mb

T = 15

What happens when the air parcel is:

brought down isothermally to p = 1000

mb

?

cooled

isobarically

to T = -10

?

raised adiabatically to p = 500

mb

?