ATMO 336 - Weather, Climate, and Society

Fall 2007 - Homework #2

 

Answer the following questions on a separate sheet of paper.  Homework answers squeezed onto this page will not be accepted.  If you need to calculate an answer, you must show your work.  To answer question 2, you will need to refer to the skew-T diagram located under the homework link on the course web page and the table of saturation mixing ratios provided with an in-class handout (referenced by temperature in Celsius).  For questions 3 and 4, you will need to use the table of saturation mixing ratios provided on the class web page under the homework link (referenced by temperature in Fahrenheit).  Use the heat index and wind chill tables (provided in lecture notes) to help answer questions 5 and 6.  Make sure you read and answer all the parts to each question!

 

1.      Suppose you were going to walk from the ocean near Calcutta, India up to the top of Mount Everest at 8846 meters above sea level.  (Round the elevation to 9000 meters).  We will look at how air temperature, pressure, and density change on your way up.

 

Elevation (meters)

Fraction of way up by altitude

Air Temperature

Air Pressure

Percentage of the atmosphere below you by weight

0

At bottom

30° C

1000 mb

0 %

3000

1/3

?

700 mb

?

6000

2/3

?

500 mb

?

9000

At top

?

330 mb

?

 

(a)    Estimate the air temperature at 3000, 6000, and 9000 meters.  The information you need to do this is contained on the lecture page entitled “Vertical variation of temperature, pressure, and density in the atmosphere.”  Do not use the rules for lifting air parcels to answer this question.

(b)    Compute the percentage of the atmosphere below 3000, 6000, and 9000 meters (based on weight).

(c)    Explain why the rate of decrease of air pressure is not constant with increasing altitude, i.e., it drops by 300 mb over the first 3000 meters of the climb (from 0 m to 3000 m), 200 mb over the next 3000 meters of the climb (from 3000 m to 6000 m), and 170 mb over the last 3000 meters of the climb (from 6000 m to 9000 m).

 

2.      You must use the skew-T diagram located under the homework link on the class web page to answer this question.  The data was taken at 0000 UTC (or 00Z) on September 7, 2006 at Vandenberg AFB in California.

(a)    What is the local Tucson date and time when this data was measured and plotted?

(b)    Fill in the missing values in the table below by reading values from the skew-T chart.  Re-write the table on your own paper.  Do not squeeze answers into the tables below.

(c)    Using the table of saturation mixing ratios (in Celsius), which was provided as part of an in-class handout, compute the relative humidity of the air at 700 mb and 500 mb.  You may round off the air temperature and dew point temperature to the nearest values in the table.

 

Air Pressure (mb)

Altitude Above Sea Level (m)

Air Temperature (°C)

Dew Point Temperature (°C)

Wind Direction

Wind Speed

(knots)

200

12430

-52

-62

East

65

250

 

 

 

 

 

300

 

 

 

 

 

400

 

 

 

 

 

500

 

 

 

 

 

700

 

 

 

----

Calm

850

 

 

 

 

 

1000

126

14

13

Southeast

5

 

3.      On a day last winter, the following conditions were measured on the UA campus.  You must use the saturation mixing ratio table (with temperature in Fahrenheit) provided under the homework link on the class web page to answer this question.

n      At 8 AM:  air temperature, T = 45° F; dew point temperature, Td = 25° F.

n      At 11 AM:  air temperature, T = 60° F; dew point temperature, Td = 25° F.

n      At 2 PM: air temperature, T = 70° F; dew point temperature, Td = 25° F.

 

(a)    Compute the relative humidity for each of the times/conditions specified above.

(b)    Explain why the relative humidity changed the way it did from 8 AM through 2 PM.  How did the water vapor content in the air change between 8 AM and 2 PM?

 

4.      Values of air temperature and relative humidity are given below for Presque Isle, Maine and Tucson, Arizona as observed on a day in spring 2004. You must use the saturation mixing ratio table (with temperature in Fahrenheit) provided under the homework link on the class web page to answer this question.

Presque Isle, Maine

Air Temperature

35° F

Relative Humidity

100 %

Weather Conditions

Rain

Tucson, Arizona

Air Temperature

90° F

Relative Humidity

25 %

Weather Conditions

Sunny

 

(a)    What are the approximate dew point temperatures at the two locations?

(b)    Of these two locations, which has the higher concentration of water vapor in the air?  How do you know?  Explain how a desert location with a low relative humidity can actually have a higher water vapor content than a location where the relative humidity is 100% with rain falling?

 

5.      On a day in summer 2004, the conditions in Tucson, Arizona and Charleston, South Carolina are given

Tucson, Arizona

Air Temperature

105° F

Relative Humidity

10 %

Charleston, South Carolina

Air Temperature

95° F

Relative Humidity

50 %

 

(a)    Using the heat index chart provided with the course lecture notes, find the heat index for the two cities.  Compare the rate of heat loss from the human body at these two locations.

 

6.      On a day last winter, conditions measured at Flagstaff, Arizona and West Yellowstone, Montana are given

 

Flagstaff, Arizona

Air Temperature

0° F

Wind Speed

20 MPH

West Yellowstone, Montana

Air Temperature

-10° F

Wind Speed

5 MPH

 

(a)    Using the wind chill chart provided with the course lecture notes, determine the wind chill equivalent temperature for Flagstaff and West Yellowstone.  Compare the rate of heat loss from the human body at these two locations.

 

7.      Evaporative cooling is one of the most ancient and one of the most energy-efficient methods of cooling a home. It long has been regarded as environmentally "safe," since the process uses no ozone-depleting chemicals, and demands one-fourth as much energy as refrigeration during the peak cooling months of the year. In dry climates such as Tucson, evaporative cooling can be used to inexpensively cool large homes.  Locally, these devices are often referred to as “swamp coolers”.  The most common form of residential evaporative cooling uses a vertical pad of absorbent cellulose fiber, a system for delivering water to the pad to keep it soaked with water, and a fan to draw air through the porous pad. As warm, dry outside air is drawn through the wet pad, water evaporates into the air, and the air gives up its heat.  In other words, energy is removed from the air in order to evaporate water. Thus, air that has moved through the wet pad is both cooler and contains more water vapor than the outdoor air.

 

The drop in temperature depends on how much water can be evaporated into the air.  This is obviously a function of relative humidity.  When the relative humidity is low, the temperature drop can be large.  However, when the relative humidity is high, the temperature drop will be small (and the swamp cooler doesn’t help much).

 

The wet bulb temperature, which was not discussed in lecture, is the lowest temperature to which air can be cooled by evaporating water into it.  This is the theoretical lower limit for the temperature of the air that comes out of an evaporative cooler.                         

 

Explain the following statements:

 

(a)    When the relative humidity is 100%, the air temperature, the dew point temperature, and the wet bulb temperature are identical.  Explain.

(b)    When the relative humidity is less than 100%, the dew point temperature and the wet bulb temperature are both lower than the air temperature.  Explain.

(c)    When the relative humidity is less than 100%, the wet bulb temperature will always be higher than the dew point temperature.  Explain.  (Hint:  What is happening to the water vapor content and dew point temperature of the air as it is being evaporatively cooled?  At what point does it become impossible to further cool air by evaporation?)