30
Chapter 5 Global Temperature (Continued) Lecture 12 2 February, 2005

Chapter 5 Global Temperature (Continued)

  • Upload
    betha

  • View
    35

  • Download
    0

Embed Size (px)

DESCRIPTION

Chapter 5 Global Temperature (Continued). Lecture 12 2 February, 2005. Land versus ocean differences. Clouds and Temperature Changes. Clouds trap net radiation in lower troposphere. Clouds reduce surface insolation. Little seasonal change in ocean surface temp. - PowerPoint PPT Presentation

Citation preview

Page 1: Chapter 5 Global Temperature  (Continued)

Chapter 5

Global Temperature (Continued)

Lecture 122 February, 2005

Page 2: Chapter 5 Global Temperature  (Continued)

Land versus ocean differences

Page 3: Chapter 5 Global Temperature  (Continued)

Clouds and Temperature Changes

Clouds reduce surface insolation

Clouds trap net radiation in

lower troposphere

Page 4: Chapter 5 Global Temperature  (Continued)

Little seasonal change in

ocean surface temp

warmest ocean waters occur in

the western tropical Pacific

notice the changes in sea

ice in the northern and

southern hemispheres

Page 5: Chapter 5 Global Temperature  (Continued)

focus on differences between the northern and southern hemispheres

why should northern Siberia

have the greatest seasonality?

why should the seasonality in N.

America be smaller than in Asia at similar

latitudes?

Difference between January & July

Page 6: Chapter 5 Global Temperature  (Continued)

Seasonal Temperature Range in Siberiathe seasonality in northern

Siberia is extreme for several reasons:

continentalitysolar angles

clear, dry air with little cloud cover (think of albedo & greenhouse

cloud effects)Verkhoyansk, Russia has a 105 °C min-max range!

Page 7: Chapter 5 Global Temperature  (Continued)

Marine and Continental Climates

WitchitaKS

San FranciscoCA

Page 8: Chapter 5 Global Temperature  (Continued)

Marine and Continental Climates

VerkhoyanskRussia

TrondheimNorway

Page 9: Chapter 5 Global Temperature  (Continued)

Gulf Stream & Temperature inWestern Europe

think of the Gulf Stream as a gigantic river of warm water in the Atlantic (moving about

6.4 kph/4 mph)the amount of water flow in this ‘river’ is

~100 sverdrups (100 million cubic meters per second)

Not exactly the whole story…

the Gulf Stream was named and partly discovered by Benjamin Franklin

Page 10: Chapter 5 Global Temperature  (Continued)

The Gulf

Stream

Page 11: Chapter 5 Global Temperature  (Continued)

The Gulf Stream and Temperatures in Western Europe

the Gulf Stream largely explains why Iceland is mostly green, even though it sits just below the

Arctic Circlevariations in the Gulf Stream have had huge implications for human societies, such as

allowing the Vikings to reach eastern Canada and the little Ice Age

water-to-land heat transfers are accomplished via latent heat transfers and

direct sensible heating of air overlying warm water

Movie: ‘The Day After Tomorrow’

Page 12: Chapter 5 Global Temperature  (Continued)

California current & temperatures

in coastal Californiawater can directly warm or

cool nearby land masses - compare California’s cool

coastal Mediterranean climate with the warm coastal climate of Italy

Page 13: Chapter 5 Global Temperature  (Continued)

Air temperature patterns

isotherm - a line connecting points of equal temperature - analogous to a line on a topo map connecting points of equal elevation

some definitions

thermal equator - a line connecting all points of highest average temperature

Page 14: Chapter 5 Global Temperature  (Continued)

notice the thermal

equator over land

notice the influence of

large mountain

ranges

Page 15: Chapter 5 Global Temperature  (Continued)
Page 16: Chapter 5 Global Temperature  (Continued)

see how isotherms

shift poleward

over continental interiors?

where would the hottest places be?

why?

Page 17: Chapter 5 Global Temperature  (Continued)

•Show energy budget animation

Page 18: Chapter 5 Global Temperature  (Continued)

Air Temperature and the Human Body

•Wind chillCorrelates cold and wind speed

•Heat indexCorrelates heat and humidity

Page 19: Chapter 5 Global Temperature  (Continued)

Wind Chill Table

Page 20: Chapter 5 Global Temperature  (Continued)

Heat Index Table

Figure 2

Page 21: Chapter 5 Global Temperature  (Continued)

Chapter 6Atmospheric and Oceanic Circulation

Concepts in this chapterair pressure

winds (global, regional, and local)global circulation systems

four driving forces in the atmosphereprimary high and low pressure areas in the atmosphere

upper air circulationocean currents & circulation

Page 22: Chapter 5 Global Temperature  (Continued)

“We live submerged at the bottom of an ocean of the element air.”

-Evangelista Torricelli

Air Pressure

Page 23: Chapter 5 Global Temperature  (Continued)

Air pressurerecall that air pressure is force per unit

area

Page 24: Chapter 5 Global Temperature  (Continued)

Ideal Gas LawP V = n R T

where R is a constantPressure*Volume = Moles*constant*Temperature

With Moles of air constant, Pressure increases

• as Volume decreases (Temperature constant)• as Temperature increases (constant Volume)

Page 25: Chapter 5 Global Temperature  (Continued)

Ideal Gas LawPV = nRT

I. pressure increases if # molecules increases (constant volume)

II. pressure increases if volume decreases (constant temperature)

III. pressure increases if temperature increases (constant volume)

Figu

re c

redi

t: ht

tp://

www.

uwsp

.edu

/geo

/facu

lty/ri

tter/g

eog1

01/te

xtbo

ok/c

ircul

atio

n/ai

r_pr

essu

re_p

_1.h

tml

I. II.

Pressure*Volume = Moles*constant*Temperature

III.

Page 26: Chapter 5 Global Temperature  (Continued)

a quick and dirty estimate of air pressure at the surface

1. define pressure: force per unit area

2. force = mass*acceleration due to gravity

(F = m g)3. mass of the atmosphere = 5x1018

kggravitational acceleration = 9.81 m s-2

4. surface area of Earth = 4R2

= 4(6,400km)2 = 5x1014 square meters5. plug it all in ….

Pressure = F / A = m g /A= 5x1018 kg * 9.81 m s-2 / 5x1014 m2

~ 100,000 kg /(m s2) Newtons per m2 (Pascal)

~ 1000 millebar (mb)

Page 27: Chapter 5 Global Temperature  (Continued)

sea level pressure = 1013 mb = 101.3 kPa = 14.5 lbs/sq. in = 29.92” mercury = 760 mm mercury = 1

atmosphere

Page 28: Chapter 5 Global Temperature  (Continued)

the weight of air literally pushes mercury up the

column

what would the column’s height be on

top of Mt. Everest?

elevation is ~8 km~ 75% of air is below

-> 0.25 * 29.92 in ~ 7.5 in

Barometer

Page 29: Chapter 5 Global Temperature  (Continued)

Pressure in the Atmosphere and Ocean

to calculate atmospheric pressure (in mb) by height (Z):

P(Z) = 1014*[1-0.0226*Z]^5.26

to calculate water pressure (in mb) by depth (D, in m):

P(D) = 100*D

Total Pressure by Depth

0

2

4

6

8

10

12

14

1013

1023

13

2036

13

3049

13

4062

13

5075

13

6088

13

7101

13

8114

13

9127

131E

+061E

+061E

+06

Pressure (mb)

Dep

th (

km)

even though gravity is pulling on both air and water, air is compressible (water

is not)

Page 30: Chapter 5 Global Temperature  (Continued)

Scuba Diving & Pressurerule of thumb in scuba diving:

Each 10 m (33 ft) increase in depth increases the pressure on every square

inch of your body by 1 atmosphere

Dive to 30 m, you have 4 atmospheres of pressure pushing on you (3 ocean + 1

atmos)