Quick Review: Pressure

Size: px
Start display at page:

Download "Quick Review: Pressure"

Transcription

1 Quick Review: Pressure The pressure force is the force exerted by an air mass on its surroundings (and vice-versa) In the atmosphere, the surroundings are usually other air masses three air masses, each exerting pressure forces on the others

2 In the atmosphere, the pressure is essentially a measure of weight. Specifically: For any given height, the pressure equals the weight of the air above that height weight pressure the pressure force from below holds the weight of the air above

3 In the atmosphere, the pressure is essentially a measure of weight. Specifically: For any given height, the pressure equals the weight of the air above that height weight And since weight is defined by weight = mass x gravity that means the pressure is really just a measure of the mass of air above that height - more mass above you means higher pressure...less mass, lower pressure pressure the pressure force from below holds the weight of the air above

4 As we move upwards in the atmosphere, the weight of the air above us (and hence the pressure) decreases - pressure decreases with height weight pressure

5 As we move upwards in the atmosphere, the weight of the air above us (and hence the pressure) decreases - pressure decreases with height weight And of course, as we go downwards, the weight of the air above us increases - so pressure increases as we move downwards pressure

6 Some things we can infer (corollaries, if you will): (1) Since pressure is determined solely by the mass of air above, the mass of air above any given pressure level (say 500 mb) must always be the same weight 500 mb pressure

7 Some things we can infer (corollaries, if you will): (1) Since pressure is determined solely by the mass of air above, the mass of air above any given pressure level (say 500 mb) must always be the same (2) By the same reasoning, given two specific pressure levels (say 500 mb and 200 mb) the mass of air between the two levels is always the same mass A mass B 200 mb 500 mb

8 Some things we can infer (corollaries, if you will): (1) Since pressure is determined solely by the mass of air above, the mass of air above any given pressure level (say 500 mb) must always be the same (2) By the same reasoning, given two specific pressure levels (say 500 mb and 200 mb) the mass of air between the two levels is always the same mass A mass B 200 mb 500 mb the weight of mass B is 300 mb regardless of temperature, time of day, season, etc.

9 Surface Pressure The surface pressure measures the weight of the whole air column, from the ground to the top of the atmosphere So...the only way to change the surface pressure is to increase or decrease the mass of the column. In particular...

10 Surface Pressure The surface pressure measures the weight of the whole air column, from the ground to the top of the atmosphere So...the only way to change the surface pressure is to increase or decrease the mass of the column. In particular... i. Air converging into the column tends to increase the surface pressure, and... convergence in the column tends to increase surface pressure

11 Surface Pressure The surface pressure measures the weight of the whole air column, from the ground to the top of the atmosphere So...the only way to change the surface pressure is to increase or decrease the mass of the column. In particular... i. Air converging into the column tends to increase the surface pressure, and... ii. Air diverging from the column tends to decrease the surface pressure divergence in the column tends to decrease surface pressure

12 But we have to be careful (Danger, Will Robinson!) because divergence at one level usually means convergence at another (and vice-versa) - (Why?)

13 But we have to be careful (Danger, Will Robinson!) because divergence at one level usually means convergence at another (and vice-versa) - (Why?) So when we talk about surface pressure changes, we really have to talk about net divergence or net convergence - Most of the time, the upper-level process wins net divergence means decreasing surface pressure

14 Surface Pressure Maps To represent surface pressure, we plot out the data on a map and draw lines (called isobars) connecting points of constant value 1006 Note that most of the time the lines go between two points Where we draw the line depends on which of the two values is closest

15 Surface Pressure Maps To represent surface pressure, we plot out the data on a map and draw lines (called isobars) connecting points of constant value 1006 Note that most of the time the lines go between two points Where we draw the line depends on which of the two values is closest

16 Surface Pressure Maps To represent surface pressure, we plot out the data on a map and draw lines (called isobars) connecting points of constant value 1006 Note that most of the time the lines go between two points Where we draw the line depends on which of the two values is closest

17 Surface Pressure Maps To represent surface pressure, we plot out the data on a map and draw lines (called isobars) connecting points of constant value 1006 Note that most of the time the lines go between two points Where we draw the line depends on which of the two values is closest

18 Let's look at this again. Suppose we're drawing the contour representing mb

19 Let's look at this again. Suppose we're drawing the contour representing mb. Well, we've got two stations with pressure equal to mb. Clearly the contour has to pass through these points

20 Let's look at this again. Suppose we're drawing the contour representing mb. Well, we've got two stations with pressure equal to mb. Clearly the contour has to pass through these points But what about in between?

21 Well, we also have stations with 1000 mb and 1006 mb. Clearly, the mb contour must go somewhere between the two. But where?

22 Well, we also have stations with 1000 mb and 1006 mb. Clearly, the mb contour must go somewhere between the two. But where? We'll assume the pressure between between the two stations changes uniformly, in the sense that halfway between the two stations in distance, the pressure is also halfway between (i.e., 1003 mb)

23 Now the full pressure difference between the stations is 6 mb, but the difference between our mb contour and the 1000 mb station (say) is only 4 mb mb 6 mb 1000

24 Now the full pressure difference between the stations is 6 mb, but the difference between our mb contour and the 1000 mb station (say) is only 4 mb. So...if the pressure changes uniformly, this tells us that the mb contour must lie a fraction of (4 mb)/(6 mb) = 2/3 of the distance between the two stations mb 6 mb 1000

25 Now the full pressure difference between the stations is 6 mb, but the difference between our mb contour and the mb station (say) is only 4 mb. So...if the pressure changes 1006 uniformly, this tells us that the mb contour must lie a fraction of (4 mb)/(6 mb) = 2/ of the distance between the two stations.

26 And of course the same reasoning applies for the other contours as well

27 And of course the same reasoning applies for the other contours as well

28 And of course the same reasoning applies for the other contours as well

29 One caveat: It's most useful to compare pressures at the same height - For surface pressure maps, this chosen height is sea level

30 One caveat: It's most useful to compare pressures at the same height - For surface pressure maps, this chosen height is sea level But dude, what if we're not at sea level? What if we live in Tibet?

31 One caveat: It's most useful to compare pressures at the same height - For surface pressure maps, this chosen height is sea level But dude, what if we're not at sea level? What if we live in Tibet? - In mountainous regions, the pressure has to be adjusted down to sea level by applying an altitude correction The correction tries to account for the weight of the air that would have been between the height of the ground (up on the mountain) and sea level

32 in mountainous regions, pressure at the ground is adjusted to give an equivalent pressure at sea level

33 In practice, surface pressure contours are usually smoothed out to highlight the big features (rather than the wiggles) surface pressure map before smoothing...and after

34 Pressure Surfaces

35 Pressure Surfaces (Not to be confused with surface pressure!)

36 Pressure Surfaces In the atmosphere, lower pressure means higher heights. Some good reference points to remember are: 200 mb: upper troposphere ( km) 500 mb: mid-troposphere (5 6 km) 850 mb: lower-troposphere (~ 1.5 km) 1000 mb: ground level (-0.25 to 0.25 km) However, the exact heights of these levels vary from place to place, and day to day

37 Suppose we're interested in where the pressure equals 500 mb in particular. On a given day, the heights where the pressure drops to 500 mb might be different at different locations (as illustrated) heights where pressure equals 500 mb above three observing stations

38 Suppose we're interested in where the pressure equals 500 mb in particular. On a given day, the heights where the pressure drops to 500 mb might be different at different locations (as illustrated) Definition: A surface in space that connects all points with a given value of pressure (say 500 mb) is called a pressure surface heights where pressure equals 500 mb above three observing stations

39 Suppose we're interested in where the pressure equals 500 mb in particular. 500 mb pressure surface On a given day, the heights where the pressure drops to 500 mb might be different at different locations (as illustrated) Definition: A surface in space that connects all points with a given value of pressure (say 500 mb) is called a pressure surface heights where pressure equals 500 mb above three observing stations

40 A pressure surface is a surface in space that connects all points with a given value of pressure (in this case 500 mb). As we'll see, the height of a pressure surface depends on the temperature.

41 Upper-Level Charts Upper-level data is usually plotted on pressure surfaces (e.g., 500 mb, 200 mb, etc) rather than at constant height levels. But instead of pressure, the 5.3 km 5.4 km 5.5 km 5.6 km contours on the plot show the height of the pressure surface above the ground (Remember, by definition, a pressure surface has the same value of pressure everywhere, which would make for a boring plot if we plotted pressure.) N E Schematic upper-level chart showing height of the 500 mb pressure surface

42 Upper-Level Charts Upper-level charts read like topographic maps, with the contours showing the height of the pressure surface...

43 A schematic upper-level chart, with contours showing the height of the 500 mb surface A' C B 5.3 km 5.4 km 5.5 km 5.6 km A N E The equivalent vertical cross-section, running along the dotted line above

44 A schematic upper-level chart, with contours showing the height of the 500 mb surface A' C B 5.3 km 5.4 km 5.5 km 5.6 km A N E height N A B C A' The equivalent vertical cross-section, running along the dotted line above

45 A schematic upper-level chart, with contours showing the height of the 500 mb surface A' C B 5.3 km 5.4 km 5.5 km 5.6 km A N E height N 5.6 km 5.3 km The equivalent vertical cross-section, running along the dotted line above A B C A'

46 A schematic upper-level chart, with contours showing the height of the 500 mb surface A' C B 5.3 km 5.4 km 5.5 km 5.6 km A N 500 mb surface E height N 5.6 km 5.3 km The equivalent vertical cross-section, running along the dotted line above A B C A'

47 South North a schematic pressure surface in 3D, with red colors showing higher heights and blue colors lower heights

48 North South the same thing as an upper-level chart, with contours showing lines of constant height

49 today's (Mon) 500 mb height chart (black contours)

50 500 mb surface A B

51 500 mb surface pressure less than 500 mb A B pressure greater than 500 mb

52 500 mb surface pressure less than 500 mb A B pressure greater than 500 mb pressure at point A is greater than pressure at point B

53 500 mb surface pressure less than 500 mb At a given altitude (such as A to B in the figure) regions of higher heights will have higher pressures, while regions of lower heights will have lower pressures And as a result... A pressure greater than 500 mb pressure at point A is greater than pressure at point B B Height contours on an upper-level chart play the same role as isobars on a surface plot. - You can think of higher height contours as higher pressure, and lower height contours as lower pressure

Quick Review: Pressure

Quick Review: Pressure Quick Review: Pressure The pressure force is the force exerted by an air mass on its surroundings (and vice-versa) In the atmosphere, the surroundings are usually other air masses three air masses, each

More information

Changes in Density Within An Air are Density Velocity Column Fixed due and/or With Respect to to Advection Divergence the Earth

Changes in Density Within An Air are Density Velocity Column Fixed due and/or With Respect to to Advection Divergence the Earth The Continuity Equation: Dines Compensation and the Pressure Tendency Equation 1. General The Continuity Equation is a restatement of the principle of Conservation of Mass applied to the atmosphere. The

More information

In this chapter, we will examine

In this chapter, we will examine In this chapter, we will examine Surface and upper level pressure charts The forces that influence the winds The equations that govern atmospheric motion Simple balanced flows Geostrophic wind (quantitative)

More information

Cyclones and Anticyclones, Ridges and Troughs

Cyclones and Anticyclones, Ridges and Troughs Cyclones and Anticyclones, Ridges and Troughs Isobars on surface maps often have a closed appearance (as illustrated) Areas of low pressure are called cyclones, while areas with high pressure are called

More information

Weather Station Model

Weather Station Model Fun with Weather Maps! (no, really stop laughing) AOSC 200 Tim Canty Class Web Site: http://www.atmos.umd.edu/~tcanty/aosc200 Topics for today: Station Model Temperature Maps Pressure Maps Fronts Lecture

More information

San Francisco State University Department of Earth & Climate Sciences. Homework 7 Key: Pressure Tendency Equation

San Francisco State University Department of Earth & Climate Sciences. Homework 7 Key: Pressure Tendency Equation San Francisco State University Department of Earth & Climate Sciences Name Homework 7 Key: Pressure Tendency Equation 1. On November 11, 2012 at 12 UTC, the 300 mb divergence over extreme southcentral

More information

The atmosphere in motion: forces and wind. AT350 Ahrens Chapter 9

The atmosphere in motion: forces and wind. AT350 Ahrens Chapter 9 The atmosphere in motion: forces and wind AT350 Ahrens Chapter 9 Recall that Pressure is force per unit area Air pressure is determined by the weight of air above A change in pressure over some distance

More information

5.5 (AIR PRESSURE) WEATHER

5.5 (AIR PRESSURE) WEATHER 1. Construct the layers of the atmosphere based on the data you re given below. Scientists know that there are four different layers. Use the information in the data chart below to draw how you think the

More information

Physics 2112 Unit 6: Electric Potential

Physics 2112 Unit 6: Electric Potential Physics 2112 Unit 6: Electric Potential Today s Concept: Electric Potential (Defined in terms of Path Integral of Electric Field) Unit 6, Slide 1 Stuff you asked about: I am very confused about the integrals

More information

Quick Questions. 1. Two charges of +1 µc each are separated by 1 cm. What is the force between them?

Quick Questions. 1. Two charges of +1 µc each are separated by 1 cm. What is the force between them? 92 3.10 Quick Questions 3.10 Quick Questions 1. Two charges of +1 µc each are separated by 1 cm. What is the force between them? 0.89 N 90 N 173 N 15 N 2. The electric field inside an isolated conductor

More information

2. Usually, the air pressure inside a building is the air pressure outside the building. a. greater than b. about the same as c.

2. Usually, the air pressure inside a building is the air pressure outside the building. a. greater than b. about the same as c. CHAPTER 5 AIR PRESSURE MULTIPLE CHOICE QUESTIONS 1. The magnitude of pressure exerted by the gas molecules composing air depends on a. the mass of the air molecules. b. the pull of gravity. c. the kinetic

More information

Remote Sensing Observations AOSC 200 Tim Canty

Remote Sensing Observations AOSC 200 Tim Canty Remote Sensing Observations AOSC 200 Tim Canty Class Web Site: http://www.atmos.umd.edu/~tcanty/aosc200 Topics for today: Maps Radar Satellite Observations Lecture 04 Feb 7 2019 1 Today s Weather Map http://www.wpc.ncep.noaa.gov/sfc/namussfcwbg.gif

More information

Fun with Weather Maps! (no, really stop laughing) AOSC 200 Tim Canty

Fun with Weather Maps! (no, really stop laughing) AOSC 200 Tim Canty Fun with Weather Maps! (no, really stop laughing) AOSC 200 Tim Canty Class Web Site: http://www.atmos.umd.edu/~tcanty/aosc200 Topics for today: Observations Station Model Temperature Maps Pressure Maps

More information

ERTH 465 Fall Lab 3. Vertical Consistency and Analysis of Thickness. (300 points)

ERTH 465 Fall Lab 3. Vertical Consistency and Analysis of Thickness. (300 points) Name Date ERTH 465 Fall 2015 Lab 3 Vertical Consistency and Analysis of Thickness (300 points) 1. All labs are to be kept in a three hole binder. Turn in the binder when you have finished the Lab. 2. Show

More information

ERTH 465 Fall Lab 5. Absolute Geostrophic Vorticity. 200 points.

ERTH 465 Fall Lab 5. Absolute Geostrophic Vorticity. 200 points. Name Date ERTH 465 Fall 2015 Lab 5 Absolute Geostrophic Vorticity 200 points. 1. All labs are to be kept in a three hole binder. Turn in the binder when you have finished the Lab. 2. Show all work in mathematical

More information

Section 2: Friction, Gravity, and Elastic Forces

Section 2: Friction, Gravity, and Elastic Forces Chapter 10, Section 2 Friction, Gravity, & Elastic Forces Section 2: Friction, Gravity, and Elastic Forces What factors determine the strength of the friction force between two surfaces? What factors affect

More information

PLOTTING WEATHER DATA to perform a SURFACE ANALYSIS

PLOTTING WEATHER DATA to perform a SURFACE ANALYSIS PLOTTING WEATHER DATA to perform a SURFACE ANALYSIS The surface analysis permits one to identify and locate the large scale features of the sea level pressure field and the surface fronts. Isobars with

More information

Final Examination. Part A Answer ONLY TWELVE QUESTIONS in Part A. (Each question is 3 points)

Final Examination. Part A Answer ONLY TWELVE QUESTIONS in Part A. (Each question is 3 points) ATS 210 Spring Term 2001 NAME: Final Examination This is a 2 hour, closed-book examination. Calculators may be used. All answers should be written on the examination paper. Use the final sheet for any

More information

OBJECTIVES: By the end of today s lesson, you will be able to. SWBAT list the layers of the atmosphere and describe the characteristics of each one.

OBJECTIVES: By the end of today s lesson, you will be able to. SWBAT list the layers of the atmosphere and describe the characteristics of each one. 7 th Grade Science Unit: Water s Cycles and Patterns Lesson: WCP 10 Name: Date: Monday, September 12, 2016 Homeroom: OBJECTIVES: By the end of today s lesson, you will be able to SWBAT list the layers

More information

ERTH 465 Fall Lab 8 Key. Absolute Geostrophic Vorticity. 200 points. 1. Answer questions with complete sentences on separate sheets.

ERTH 465 Fall Lab 8 Key. Absolute Geostrophic Vorticity. 200 points. 1. Answer questions with complete sentences on separate sheets. Name Date ERTH 465 Fall 2017 Lab 8 Key Absolute Geostrophic Vorticity 200 points. 1. Answer questions with complete sentences on separate sheets. 2. Show all work in mathematical problems. No credit given

More information

Graphing Review Part 1: Circles, Ellipses and Lines

Graphing Review Part 1: Circles, Ellipses and Lines Graphing Review Part : Circles, Ellipses and Lines Definition The graph of an equation is the set of ordered pairs, (, y), that satisfy the equation We can represent the graph of a function by sketching

More information

Chemical Applications of Symmetry and Group Theory Prof. Manabendra Chandra Department of Chemistry Indian Institute of Technology, Kanpur

Chemical Applications of Symmetry and Group Theory Prof. Manabendra Chandra Department of Chemistry Indian Institute of Technology, Kanpur Chemical Applications of Symmetry and Group Theory Prof. Manabendra Chandra Department of Chemistry Indian Institute of Technology, Kanpur Lecture - 09 Hello, welcome to the day 4 of our second week of

More information

Plasma Physics Prof. V. K. Tripathi Department of Physics Indian Institute of Technology, Delhi

Plasma Physics Prof. V. K. Tripathi Department of Physics Indian Institute of Technology, Delhi Plasma Physics Prof. V. K. Tripathi Department of Physics Indian Institute of Technology, Delhi Module No. # 01 Lecture No. # 22 Adiabatic Invariance of Magnetic Moment and Mirror Confinement Today, we

More information

Calculus 140, section 4.7 Concavity and Inflection Points notes by Tim Pilachowski

Calculus 140, section 4.7 Concavity and Inflection Points notes by Tim Pilachowski Calculus 140, section 4.7 Concavity and Inflection Points notes by Tim Pilachowski Reminder: You will not be able to use a graphing calculator on tests! Theory Eample: Consider the graph of y = pictured

More information

Now that we know, more or less, what air is made of, let's talk a bit about it's physical properties.

Now that we know, more or less, what air is made of, let's talk a bit about it's physical properties. Now that we know, more or less, what air is made of, let's talk a bit about it's physical properties. Meditations on a Glass of Water Think about a glass of water for a minute. Depending on how you look

More information

Characteristics of the Atmosphere

Characteristics of the Atmosphere Characteristics of the Atmosphere * The atmosphere is a mixture of gases that surrounds the Earth. * It contains oxygen and protects us from the sun's ultraviolet rays. * The atmosphere has 78% Nitrogen,

More information

Advanced Hydrology Prof. Dr. Ashu Jain Department of Civil Engineering Indian Institute of Technology, Kanpur. Lecture - 13

Advanced Hydrology Prof. Dr. Ashu Jain Department of Civil Engineering Indian Institute of Technology, Kanpur. Lecture - 13 Advanced Hydrology Prof. Dr. Ashu Jain Department of Civil Engineering Indian Institute of Technology, Kanpur Lecture - 13 Good morning friends and welcome to the video course on Advanced Hydrology. In

More information

Characteristics of the Atmosphere

Characteristics of the Atmosphere Characteristics of the Atmosphere * The atmosphere is a mixture of gases that surrounds the Earth. * It contains oxygen and protects us from the sun's ultraviolet rays. * The atmosphere has 78% Nitrogen,

More information

MITOCW 5. Traveling Waves without Damping

MITOCW 5. Traveling Waves without Damping MITOCW 5. Traveling Waves without Damping The following content is provided under a Creative Commons license. Your support will help MIT OpenCourseWare continue to offer high-quality educational resources

More information

I. Convective Available Potential Energy (CAPE)

I. Convective Available Potential Energy (CAPE) Reading 4: Procedure Summary-- Calcluating CAPE, Lifted Index and Strength of Maximum Convective Updraft CAPE Calculation Lifted Index Calculation Maximum Updraft Strength Calculation I. Convective Available

More information

Tides Unit II: The Bulge Theory of the Tides (3.5 pts)

Tides Unit II: The Bulge Theory of the Tides (3.5 pts) T. James Noyes, ECC Tides Unit II: The Bulge Theory of the Tides (Topic 7A-2) page 1 Name: Section: Tides Unit II: The Bulge Theory of the Tides (3.5 pts) The Bulge Theory of the Tides is the Simplest,

More information

MITOCW watch?v=pqkyqu11eta

MITOCW watch?v=pqkyqu11eta MITOCW watch?v=pqkyqu11eta The following content is provided under a Creative Commons license. Your support will help MIT OpenCourseWare continue to offer high quality educational resources for free. To

More information

I. Convective Available Potential Energy (CAPE)

I. Convective Available Potential Energy (CAPE) Calculating CAPE, Lifted Index and Strength of Maximum Convective Updraft CAPE Calculation Lifted Index Calculation Maximum Updraft Strength Calculation I. Convective Available Potential Energy (CAPE)

More information

Problem Solving: Faraday s Law & Inductance. Faraday s Law

Problem Solving: Faraday s Law & Inductance. Faraday s Law MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics: 8.02 Problem Solving: Faraday s Law & Inductance Section Table Names Faraday s Law In Chapter 10 of the 8.02 Course Notes, we have seen that

More information

Gravity and Orbits. 1. Choose the picture you think shows the gravity forces on the Earth and the Sun.

Gravity and Orbits. 1. Choose the picture you think shows the gravity forces on the Earth and the Sun. Name: Grade: Gravity and Orbits Pre-lab 1. Choose the picture you think shows the gravity forces on the Earth and the Sun. (a longer arrow to represents a big force, and a shorter arrow represent a smaller

More information

4 Forecasting Weather

4 Forecasting Weather CHAPTER 16 4 Forecasting Weather SECTION Understanding Weather BEFORE YOU READ After you read this section, you should be able to answer these questions: What instruments are used to forecast weather?

More information

Electro Magnetic Field Dr. Harishankar Ramachandran Department of Electrical Engineering Indian Institute of Technology Madras

Electro Magnetic Field Dr. Harishankar Ramachandran Department of Electrical Engineering Indian Institute of Technology Madras Electro Magnetic Field Dr. Harishankar Ramachandran Department of Electrical Engineering Indian Institute of Technology Madras Lecture - 7 Gauss s Law Good morning. Today, I want to discuss two or three

More information

Maps and Remote Sensing AOSC 200 Tim Canty

Maps and Remote Sensing AOSC 200 Tim Canty Maps and Remote Sensing AOSC 200 Tim Canty Class Web Site: http://www.atmos.umd.edu/~tcanty/aosc200 Topics for today: Weather Maps Radar Satellite Observations Lecture 04 Feb 7 2019 1 Today s Weather Map

More information

MITOCW MIT8_01F16_w02s05v06_360p

MITOCW MIT8_01F16_w02s05v06_360p MITOCW MIT8_01F16_w02s05v06_360p One of our classic problems to analyze using Newton's second law is the motion of two blocks with a rope that's wrapped around a pulley. So imagine we have a pulley, P,

More information

Special Theory of Relativity Prof. Shiva Prasad Department of Physics Indian Institute of Technology, Bombay

Special Theory of Relativity Prof. Shiva Prasad Department of Physics Indian Institute of Technology, Bombay Special Theory of Relativity Prof. Shiva Prasad Department of Physics Indian Institute of Technology, Bombay Lecture - 24 Current Density Four Vector and Maxwell Equation Hello, so we have now come to

More information

Please read this introductory material carefully; it covers topics you might not yet have seen in class.

Please read this introductory material carefully; it covers topics you might not yet have seen in class. b Lab Physics 211 Lab 10 Torque What You Need To Know: Please read this introductory material carefully; it covers topics you might not yet have seen in class. F (a) (b) FIGURE 1 Forces acting on an object

More information

MITOCW MIT8_01F16_L12v01_360p

MITOCW MIT8_01F16_L12v01_360p MITOCW MIT8_01F16_L12v01_360p Let's look at a typical application of Newton's second law for a system of objects. So what I want to consider is a system of pulleys and masses. So I'll have a fixed surface

More information

The magnitude of this force is a scalar quantity called weight.

The magnitude of this force is a scalar quantity called weight. Everyday Forces has direction The gravitational force (F g ) exerted on the ball by Earth is a vector directed toward the center of the earth. The magnitude of this force is a scalar quantity called weight.

More information

Electric Field. Purpose of the experiment. PES 2160 Advanced Physics Lab II

Electric Field. Purpose of the experiment. PES 2160 Advanced Physics Lab II Electric Field PES 2160 Advanced Physics Lab II Purpose of the experiment To see what an electric field and electric potential look like. To understand how the shape of the electric field and potential

More information

PRACTICAL ACTIVITY: DRAWING ISOLINES OR CONTOURS

PRACTICAL ACTIVITY: DRAWING ISOLINES OR CONTOURS COME RAIN OR SHINE PRACTICAL ACTIVITY: DRAWING ISOLINES OR CONTOURS Ideally you would need a pencil for this activity (rather than a pen) and coloured pencils are useful too. These activities maybe a little

More information

Regents Earth Science Unit 1 Earth Dimensions

Regents Earth Science Unit 1 Earth Dimensions Regents Earth Science Unit 1 Earth Dimensions www. BarnesWeb.org 2014-15 edition Name: Name: OBJECTIVES Correctly define: isolines, gradient, topographic map, contour interval, hachured lines, profile,

More information

WO2 ROZSA-HRABINSKI METEOROLOGY 1

WO2 ROZSA-HRABINSKI METEOROLOGY 1 WO2 ROZSA-HRABINSKI METEOROLOGY 1 INTRODUCTION What are we covering today? The Atmosphere Clouds Atmospheric Stability Temperature and Humidity THE ATMOSPHERE THE ATMOSPHERE The atmosphere is composed

More information

You Might Also Like. I look forward helping you focus your instruction while saving tons of time. Kesler Science Station Lab Activities 40%+ Savings!

You Might Also Like. I look forward helping you focus your instruction while saving tons of time. Kesler Science Station Lab Activities 40%+ Savings! Thanks Connect Thank you for downloading my product. I truly appreciate your support and look forward to hearing your feedback. You can connect with me and find many free activities and strategies over

More information

Lecture 1. Equations of motion - Newton s second law in three dimensions. Pressure gradient + force force

Lecture 1. Equations of motion - Newton s second law in three dimensions. Pressure gradient + force force Lecture 3 Lecture 1 Basic dynamics Equations of motion - Newton s second law in three dimensions Acceleration = Pressure Coriolis + gravity + friction gradient + force force This set of equations is the

More information

Isentropic Analysis. We can look at weather data in other ways besides on constantpressure. Meteorology 411 Iowa State University Week 11 Bill Gallus

Isentropic Analysis. We can look at weather data in other ways besides on constantpressure. Meteorology 411 Iowa State University Week 11 Bill Gallus Isentropic Analysis We can look at weather data in other ways besides on constantpressure surfaces! Meteorology 411 Iowa State University Week 11 Bill Gallus A brief history of meteorology In the 1930s

More information

Lesson 6-1: Relations and Functions

Lesson 6-1: Relations and Functions I ll bet you think numbers are pretty boring, don t you? I ll bet you think numbers have no life. For instance, numbers don t have relationships do they? And if you had no relationships, life would be

More information

Solving with Absolute Value

Solving with Absolute Value Solving with Absolute Value Who knew two little lines could cause so much trouble? Ask someone to solve the equation 3x 2 = 7 and they ll say No problem! Add just two little lines, and ask them to solve

More information

Fall 2015 Laboratory 7 Quasigeostrophic Forcing Functions 300 points. You are provided with the following for 12 UTC 12/4/12 (a) WRF-NAM

Fall 2015 Laboratory 7 Quasigeostrophic Forcing Functions 300 points. You are provided with the following for 12 UTC 12/4/12 (a) WRF-NAM ERTH 465 Fall 2015 Laboratory 7 NAME Quasigeostrophic Forcing Functions 300 points. You are provided with the following for 12 UTC 12/4/12 (a) WRF-NAM initialization of SLP and 1000-500 mb thickness; (b)

More information

Section 1.1: Patterns in Division

Section 1.1: Patterns in Division Section 1.1: Patterns in Division Dividing by 2 All even numbers are divisible by 2. E.g., all numbers ending in 0,2,4,6 or 8. Dividing by 4 1. Are the last two digits in your number divisible by 4? 2.

More information

Physics 9 Monday, November 26, 2018

Physics 9 Monday, November 26, 2018 Physics 9 Monday, November 26, 2018 HW10 due this Friday. For today, you read Giancoli ch19 (DC circuits) For Wednesday, read Mazur ch31 (electric circuits) The main goals for the electricity segment (the

More information

Quasi-Geostrophic ω-equation. 1. The atmosphere is approximately hydrostatic. 2. The atmosphere is approximately geostrophic.

Quasi-Geostrophic ω-equation. 1. The atmosphere is approximately hydrostatic. 2. The atmosphere is approximately geostrophic. Quasi-Geostrophic ω-equation For large-scale flow in the atmosphere, we have learned about two very important characteristics:. The atmosphere is approximately hydrostatic.. The atmosphere is approximately

More information

Force, Friction & Gravity Notes

Force, Friction & Gravity Notes Force, Friction & Gravity Notes Key Terms to Know Speed: The distance traveled by an object within a certain amount of time. Speed = distance/time Velocity: Speed in a given direction Acceleration: The

More information

Electromagnetic Theory Prof. D. K. Ghosh Department of Physics Indian Institute of Technology, Bombay

Electromagnetic Theory Prof. D. K. Ghosh Department of Physics Indian Institute of Technology, Bombay Electromagnetic Theory Prof. D. K. Ghosh Department of Physics Indian Institute of Technology, Bombay Module - 4 Time Varying Field Lecture - 30 Maxwell s Equations In the last lecture we had introduced

More information

MA 102 Mathematics II Lecture Feb, 2015

MA 102 Mathematics II Lecture Feb, 2015 MA 102 Mathematics II Lecture 1 20 Feb, 2015 Differential Equations An equation containing derivatives is called a differential equation. The origin of differential equations Many of the laws of nature

More information

Kind of plate boundary (convergent or divergent?)

Kind of plate boundary (convergent or divergent?) 19B Plate Tectonics What is plate tectonics? Earth s crust plus the upper mantle forms the lithosphere. Earth s lithosphere is broken in a number of different pieces. How these pieces move and interact

More information

Chapter 20 & 21: Electrostatics

Chapter 20 & 21: Electrostatics There are four forces that exist in nature: 1. 2. 3. 4. Chapter 20 & 21: Electrostatics, that is, they only act over very small distances. and can act over very large distances. Rules of Electrostatics:

More information

Surveying Prof. Bharat Lohani Department of Civil Engineering Indian Institute of Technology, Kanpur. Module - 4 Lecture - 1 Compass Surveying

Surveying Prof. Bharat Lohani Department of Civil Engineering Indian Institute of Technology, Kanpur. Module - 4 Lecture - 1 Compass Surveying Surveying Prof. Bharat Lohani Department of Civil Engineering Indian Institute of Technology, Kanpur Module - 4 Lecture - 1 Compass Surveying Welcome to this video lecture series on basic surveying and

More information

Physics E-1ax, Fall 2014 Experiment 3. Experiment 3: Force. 2. Find your center of mass by balancing yourself on two force plates.

Physics E-1ax, Fall 2014 Experiment 3. Experiment 3: Force. 2. Find your center of mass by balancing yourself on two force plates. Learning Goals Experiment 3: Force After you finish this lab, you will be able to: 1. Use Logger Pro to analyze video and calculate position, velocity, and acceleration. 2. Find your center of mass by

More information

TEACHER BACKGROUND INFORMATION FORCE

TEACHER BACKGROUND INFORMATION FORCE TEACHER BACKGROUND INFORMATION FORCE WHAT IS FORCE? Force is anything that can change the state of motion of a body. In simpler terms, force is a push or a pull. For example, wind pushing on a flag is

More information

ESS15 Lecture 10. Winds and weather The Coriolis force Global circulations of atmosphere & ocean Weather vs. Climate

ESS15 Lecture 10. Winds and weather The Coriolis force Global circulations of atmosphere & ocean Weather vs. Climate ESS15 Lecture 10 Winds and weather The Coriolis force Global circulations of atmosphere & ocean Weather vs. Climate Earth s energy imbalances, winds, and the global circulation of the atmopshere. Please

More information

Analyzing/Forecasting Weather

Analyzing/Forecasting Weather Analyzing/Forecasting Weather Focus Question Dude Its wind. It blows everywhere. Meteorologist to Nicholas Cage in The Weatherman VA SOL SOL 3 The student will investigate and understand how to read and

More information

Surveying Prof. Bharat Lohani Department of Civil Engineering Indian Institute of Technology, Kanpur. Module - 3 Lecture - 4 Linear Measurements

Surveying Prof. Bharat Lohani Department of Civil Engineering Indian Institute of Technology, Kanpur. Module - 3 Lecture - 4 Linear Measurements Surveying Prof. Bharat Lohani Department of Civil Engineering Indian Institute of Technology, Kanpur Module - 3 Lecture - 4 Linear Measurements Welcome again to this another video lecture on basic surveying.

More information

Lesson 2-6: Graphs of Absolute Value Equations

Lesson 2-6: Graphs of Absolute Value Equations Where we re headed today Today we re going to take the net graphing step we ll learn how to graph absolute value equations. Here are the three things you are going to need to be able to do: 1. Match an

More information

Hydrostatics and Stability Dr. Hari V Warrior Department of Ocean Engineering and Naval Architecture Indian Institute of Technology, Kharagpur

Hydrostatics and Stability Dr. Hari V Warrior Department of Ocean Engineering and Naval Architecture Indian Institute of Technology, Kharagpur Hydrostatics and Stability Dr. Hari V Warrior Department of Ocean Engineering and Naval Architecture Indian Institute of Technology, Kharagpur Module No. # 01 Lecture No. # 09 Free Surface Effect In the

More information

[5] SA1.2 The student demonstrates an understanding of the processes of science by using

[5] SA1.2 The student demonstrates an understanding of the processes of science by using Overview: Students learn the composition and layers of the atmosphere through discussion, creation of a scale model, and a written exercise. (NOTE: This lesson may require more than one class period. Students

More information

Forces and Newton s Laws Reading Notes. Give an example of a force you have experienced continuously all your life.

Forces and Newton s Laws Reading Notes. Give an example of a force you have experienced continuously all your life. Forces and Newton s Laws Reading Notes Name: Section 4-1: Force What is force? Give an example of a force you have experienced continuously all your life. Give an example of a situation where an object

More information

Chapter 2. Kinematic Equations. Problem 1. Kinematic Equations, specific. Motion in One Dimension

Chapter 2. Kinematic Equations. Problem 1. Kinematic Equations, specific. Motion in One Dimension Kinematic Equations Chapter Motion in One Dimension The kinematic equations may be used to solve any problem involving one-dimensional motion with a constant You may need to use two of the equations to

More information

Free-Body Diagrams: Introduction

Free-Body Diagrams: Introduction Free-Body Diagrams: Introduction Learning Goal: To learn to draw free-body diagrams for various real-life situations. Imagine that you are given a description of a real-life situation and are asked to

More information

Chapter 5: Preferences

Chapter 5: Preferences Chapter 5: Preferences 5.1: Introduction In chapters 3 and 4 we considered a particular type of preferences in which all the indifference curves are parallel to each other and in which each indifference

More information

Fluids in Rigid Body Motion

Fluids in Rigid Body Motion Fluids in Rigid Body Motion Introduction Recall, for the case of rigid body motion, the equation of motion for fluid flow (the Navier-Stokes equation) reduces to Note that a new "effective gravity" vector,

More information

Summary of High Wind Event of 7 March 2004

Summary of High Wind Event of 7 March 2004 Summary of High Wind Event of 7 March 2004 This event was characterized by a very strong jet streak that developed over North Carolina by 00 UTC 8 March, as seen in the Eta model analysis at 300 mb, with

More information

Chapter 1 Review of Equations and Inequalities

Chapter 1 Review of Equations and Inequalities Chapter 1 Review of Equations and Inequalities Part I Review of Basic Equations Recall that an equation is an expression with an equal sign in the middle. Also recall that, if a question asks you to solve

More information

NATS 101. Lecture 15 Surface and Upper-Air Maps

NATS 101. Lecture 15 Surface and Upper-Air Maps NATS 101 Lecture 15 Surface and Upper-Air Maps Due Today Turn in 4 by 6 card, include Comments on Lecture PIN (Optional) Signature (Mandatory and Legible) Supplemental References for Today s s Lecture

More information

GRAVITATIONAL FORCE NEAR EARTH

GRAVITATIONAL FORCE NEAR EARTH GRAVITATIONAL FORCE NEAR EARTH Recap: Gravitational Force Field Recall that gravity is an action-at-adistance force that pulls on objects (regardless of their size or mass) without making any contact with

More information

Tectonic Forces Simulation: Volcanoes Activity One

Tectonic Forces Simulation: Volcanoes Activity One Tectonic Forces Simulation: Volcanoes Activity One Introduction Volcanoes form above vents or cracks in the earth's crust. When a volcano erupts, magma is forced up through the cracks - sending lava, ash,

More information

The Behaviour of the Atmosphere

The Behaviour of the Atmosphere 3 The Behaviour of the Atmosphere Learning Goals After studying this chapter, students should be able to: apply the ideal gas law and the concept of hydrostatic balance to the atmosphere (pp. 49 54); apply

More information

Go With the Flow From High to Low Investigating Isobars

Go With the Flow From High to Low Investigating Isobars Go With the Flow From High to Low Investigating Isobars Science 10 Mrs. Purba Air Masses The air over a warm surface can be heated, causing it to rise above more dense air. The result is the formation

More information

Appendix B Lesson 1: What Is Weather Exit Ticket

Appendix B Lesson 1: What Is Weather Exit Ticket Appendix B Lesson 1: What Is Weather Exit Ticket Name Date Period What is Weather? Exit Ticket List 3 things that you learned during the demonstrations today. What are two questions that you still have?

More information

Let's See What we can Remember?

Let's See What we can Remember? Let's See What we can Remember? * What is Acceleration? A change in velocity * How do you determine an objects velocity? Speed & Direction * What is speed? How fast an objects position is changing *What

More information

The First Derivative Test

The First Derivative Test The First Derivative Test We have already looked at this test in the last section even though we did not put a name to the process we were using. We use a y number line to test the sign of the first derivative

More information

Suppose that f is continuous on [a, b] and differentiable on (a, b). Then

Suppose that f is continuous on [a, b] and differentiable on (a, b). Then Lectures 1/18 Derivatives and Graphs When we have a picture of the graph of a function f(x), we can make a picture of the derivative f (x) using the slopes of the tangents to the graph of f. In this section

More information

Line Integrals and Path Independence

Line Integrals and Path Independence Line Integrals and Path Independence We get to talk about integrals that are the areas under a line in three (or more) dimensional space. These are called, strangely enough, line integrals. Figure 11.1

More information

Measuring Keepers S E S S I O N 1. 5 A

Measuring Keepers S E S S I O N 1. 5 A S E S S I O N 1. 5 A Measuring Keepers Math Focus Points Naming, notating, and telling time to the hour on a digital and an analog clock Understanding the meaning of at least in the context of linear measurement

More information

Lecture 6 Force and Motion. Identifying Forces Free-body Diagram Newton s Second Law

Lecture 6 Force and Motion. Identifying Forces Free-body Diagram Newton s Second Law Lecture 6 Force and Motion Identifying Forces Free-body Diagram Newton s Second Law We are now moving on from the study of motion to studying what causes motion. Forces are what cause motion. Forces are

More information

Chapter 3 Acceleration

Chapter 3 Acceleration Chapter 3 Acceleration Slide 3-1 PackBack The first answer gives a good physical picture. The video was nice, and worth the second answer. https://www.youtube.com/w atch?v=m57cimnj7fc Slide 3-2 Slide 3-3

More information

ERTH 465 Fall Lab 3. Vertical Consistency and Analysis of Thickness

ERTH 465 Fall Lab 3. Vertical Consistency and Analysis of Thickness Name Date ERTH 465 Fall 2015 Lab 3 Vertical Consistency and Analysis of Thickness 1. All labs are to be kept in a three hole binder. Turn in the binder when you have finished the Lab. 2. Show all work

More information

The hitch in all of this is figuring out the two principal angles and which principal stress goes with which principal angle.

The hitch in all of this is figuring out the two principal angles and which principal stress goes with which principal angle. Mohr s Circle The stress basic transformation equations that we developed allowed us to determine the stresses acting on an element regardless of its orientation as long as we know the basic stresses σx,

More information

1 Least Squares Estimation - multiple regression.

1 Least Squares Estimation - multiple regression. Introduction to multiple regression. Fall 2010 1 Least Squares Estimation - multiple regression. Let y = {y 1,, y n } be a n 1 vector of dependent variable observations. Let β = {β 0, β 1 } be the 2 1

More information

Mathematician Preemptive Strike 2 Due on Day 1 of Chapter 2

Mathematician Preemptive Strike 2 Due on Day 1 of Chapter 2 Mathematician Preemptive Strike Due on Day 1 of Chapter Your first experience with a Wiggle chart. Not to be confused with anything related to the Wiggles Note: It s also called a Sign chart, but since

More information

Do Now. Copy the ques:on below and write down an. Sketch a profile of the books on the front table.

Do Now. Copy the ques:on below and write down an. Sketch a profile of the books on the front table. Do Now Copy the ques:on below and write down an answer Sketch a profile of the books on the front table. Measurements Contour Lines How do we represent Eleva:on on a flat piece of paper? Eleva?on height

More information

Section - 9 GRAPHS. (a) y f x (b) y f x. (c) y f x (d) y f x. (e) y f x (f) y f x k. (g) y f x k (h) y kf x. (i) y f kx. [a] y f x to y f x

Section - 9 GRAPHS. (a) y f x (b) y f x. (c) y f x (d) y f x. (e) y f x (f) y f x k. (g) y f x k (h) y kf x. (i) y f kx. [a] y f x to y f x 44 Section - 9 GRAPHS In this section, we will discuss graphs and graph-plotting in more detail. Detailed graph plotting also requires a knowledge of derivatives. Here, we will be discussing some general

More information

Mapping Earth Review Note Cards

Mapping Earth Review Note Cards Review Note Cards Spheres of Earth Atmosphere- Layer of gases Hydrosphere- All liquid water Lithosphere- Solid surface Biosphere-Living Portion Cryosphere-Ice Portion Evidence that the Earth is Round The

More information

Forces. A force is a push or a pull on an object

Forces. A force is a push or a pull on an object Forces Forces A force is a push or a pull on an object Arrows are used to represent forces. The direction of the arrow represent the direction the force that exist or being applied. Forces A net force

More information

Question: How do we use a Hertzsprung-Russell Diagram to explain star characteristics?

Question: How do we use a Hertzsprung-Russell Diagram to explain star characteristics? The Hertzsprung-Russell Diagram Assignment Introduction: The development of the H-R Diagram began with Danish astronomer Ejnar Hertzsprung who began plotting the stars around 1911. American astronomer

More information

Chapter 19 Electric Potential and Electric Field Sunday, January 31, Key concepts:

Chapter 19 Electric Potential and Electric Field Sunday, January 31, Key concepts: Chapter 19 Electric Potential and Electric Field Sunday, January 31, 2010 10:37 PM Key concepts: electric potential electric potential energy the electron-volt (ev), a convenient unit of energy when dealing

More information