Figure 1: You and Your Elephant

Similar documents
Notes Chapter 3. Buoyancy

Chapter 10 Fluids. Which has a greater density? Ch 10: Problem 5. Ch 10: Problem Phases of Matter Density and Specific Gravity

Fluid Mechanics. Liquids and gases have the ability to flow They are called fluids There are a variety of LAWS that fluids obey

Density and Specific Gravity

PHYS 101 Previous Exam Problems

From and

Fluids: Floating & Flying. Student Leaning Objectives 2/16/2016. Distinguish between force and pressure. Recall factors that allow floating

Fluids. James H Dann, Ph.D. Say Thanks to the Authors Click (No sign in required)

Density and Buoyancy Notes

Unit 7. Pressure in fluids

Chapter 13 Fluids. Copyright 2009 Pearson Education, Inc.

. In an elevator accelerating upward (A) both the elevator accelerating upward (B) the first is equations are valid

Why do things float? Climate and Global Change. Introduction

Chapter 9. Forces and Fluids

Up Up and Away on Beautiful Balloons: Scaling up from Party Favors to Scientific Payloads

Types of Forces. Pressure Buoyant Force Friction Normal Force

Unit 1 Lesson 5 Fluids and Pressure. Copyright Houghton Mifflin Harcourt Publishing Company

Lecture 29 (Walker: ) Fluids II April 13, 2009

3. How many kilograms of air is in the room?

3. A fluid is forced through a pipe of changing cross section as shown. In which section would the pressure of the fluid be a minimum?

Page 1. Balance of Gravity Energy More compressed at sea level than at higher altitudes Moon has no atmosphere

Float a Big Stick. To investigate how objects float by analyzing forces acting on a floating stick

Chapter 9 Fluids and Buoyant Force

L 13 Fluid Statics [2] More on fluids. How can a steel boat float. A ship can float in a cup of water! Today s weather

PHYSICS - CLUTCH CH 17: FLUID MECHANICS.

PHYS:1200 LECTURE 13 FLUIDS (2)

Gases and Pressure SECTION 11.1

Additional Information

Fluids always move from high pressure to low pressure. Air molecules pulled by gravity = atmospheric pressure

Chapter 15 Fluid. Density

Chapter 13 Fluids. Copyright 2009 Pearson Education, Inc.

Chapter Five: Density and Buoyancy

Today: Finish Chapter 13 (Liquids) Start Chapter 14 (Gases and Plasmas)

5.0 Neutral Buoyancy Test

In the liquid phase, molecules can flow freely from position to position by sliding over one another. A liquid takes the shape of its container.

UNIT 2 FLUIDS PHYS:1200 LECTURE 12 FLUIDS (1)

Science 8 Chapter 9 Section 1

Card 1 Chapter 17. Card 2. Chapter 17

Grade 8 Science: Unit 2-Fluids Chapter 9: Force, Pressure Area

Chapter 13 Fluids. Copyright 2009 Pearson Education, Inc.

Unit A-2: List of Subjects

1 Fluids and Pressure

Phys101 Lectures Fluids I. Key points: Pressure and Pascal s Principle Buoyancy and Archimedes Principle. Ref: 10-1,2,3,4,5,6,7.

In the liquid phase, molecules can flow freely from position. another. A liquid takes the shape of its container. 19.

Name. Student I.D.. Section:. Use g = 10 m/s 2

Hydrostatics. Physics 1425 Lecture 25. Michael Fowler, UVa

ConcepTest PowerPoints

Exercises The Atmosphere (page 383) 20.2 Atmospheric Pressure (pages )

Example A: A 400-N force is applied to a tabletop over a square area with side-length L = 20-cm.

Density, Pressure Learning Outcomes

DIVING PHYSICS EXAMPLE QUESTIONS

Fluid Mechanics - Hydrostatics. Sections 11 5 and 6

Enter your parameter set number (1-27)

Vacuum P=0. h=76 cm A B C. Barometer

CHAPTER 31 IDEAL GAS LAWS

2 Buoyant Force. TAKE A LOOK 2. Identify What produces buoyant force?

Student Exploration: Archimedes Principle

Pressure is defined as force per unit area. Any fluid can exert a force

Matter is made up of particles which are in continual random motion Misconception: Only when a substance is in its liquid or gas state do its

Chapter 15 Fluids. Copyright 2010 Pearson Education, Inc.

Density. Chapters 12-14: Phases of Matter. Example: Density. Conceptual Check. Springs 2/27/12. Mass Density vs. Weight Density

Scott Denning CSU CMMAP 1

1/4/18. Density. Density. Density

28 multiple choice, 4 wrong answers will be dropped Covers everything learned in Phys 105 and 106

Clicker Question: Clicker Question: Clicker Question: Phases of Matter. Phases of Matter and Fluid Mechanics

Density, Pressure Learning Outcomes

FC-CIV HIDRCANA: Channel Hydraulics Flow Mechanics Review Fluid Statics

Lecture Outline Chapter 15. Physics, 4 th Edition James S. Walker. Copyright 2010 Pearson Education, Inc.

End of Chapter Exercises

Balloon Calculations

2015 EdExcel A Level Physics Topic 4. Density and upthrust

3 1 PRESSURE. This is illustrated in Fig. 3 3.

When a uniform pressure acts on a flat plate of area A and a force F pushes the plate, then the pressure p is : p = F/A

Chapter 13 Gases, Vapors, Liquids, and Solids

Static Fluids. **All simulations and videos required for this package can be found on my website, here:

Page 1

Name Class Date. (pp ) Write the letter of the correct answer in the space provided.

Process Nature of Process

Lecture 19 Fluids: density, pressure, Pascal s principle and Buoyancy.

Fluids, Pressure and buoyancy

More About Solids, Liquids and Gases ASSIGNMENT

COURSE NUMBER: ME 321 Fluid Mechanics I Fluid statics. Course teacher Dr. M. Mahbubur Razzaque Professor Department of Mechanical Engineering BUET

10.4 Buoyancy is a force

Please pick up your midterm if you haven t already. Today: Finish Chapter 13 (Liquids) from last time. Start Chapter 14 (Gases and Plasmas)

Fluids. How do fluids exert pressure? What causes objects to float? What happens when pressure in a fluid changes? What affects the speed of a fluid?

PHY131H1S - Class 23. Today: Fluids Pressure Pascal s Law Gauge Pressure Buoyancy, Archimedes Principle. A little pre-class reading quiz

Please welcome for any correction or misprint in the entire manuscript and your valuable suggestions kindly mail us

Phys101 Lectures Fluids I. Key points: Pressure and Pascal s Principle Buoyancy and Archimedes Principle. Ref: 10-1,2,3,4,5,6,7.

Force Pressure = Area

Objectives deals with forces applied by fluids at rest or in rigid-body motion.

Unit 9 Packet: Gas Laws Introduction to Gas Laws Notes:

L-14 Fluids [3] Buoyancy why things float. Buoyant Force F B. Archimedes principle. Archimedes Principle

End of Chapter Exercises

LECTURE 16: Buoyancy. Select LEARNING OBJECTIVES:

Physics 152: Homework Problems on Fluids

Conceptual Physics Fundamentals

Activity 4 Buoyancy in a Liquid /Archimedes' Principle F1003 Physics II ITESM Campus Aguascalientes January-May 2017 Dr. Juan-Manuel CAMPOS-SANDOVAL

The Language of Physics

Flying High. HHJS Science Week Background Information. Forces and Flight

EXPERIMENT 8 BUOYANT FORCES

Transcription:

INSTRUCTORS NOTE (Dr. Jack Blumenthal) The thought experiment or problem described herein, together with the accompanying approach and calculations was developed by two seniors and their instructor at Mayfield Senior School in Pasadena, California as part of a special study program introducing engineering thermodynamics. We feel that this problem which requires physics, chemistry, and math elements is a very nice project for students who are taking or have taken courses in chemistry, physics and calculus.. THE PROBLEM SO HOW HIGH WILL YOUR ELEPHANT FLY? By Jack Blumenthal, Rafaela Bradvica, Katherine Karl Congratulations, you got a baby elephant (500 kg) for Christmas and you want to design a spherical, helium filled balloon that will just lift your elephant and you (50kg) at sea level when the atmospheric pressure is 101.3 kpa and the temperature is 288K. After you have designed and built the balloon, and you and your elephant have gotten onto the platform (see figure 1), the balloon just floats at sea level (it neither rises or falls). Suddenly your elephant pushes you off of the platform and your balloon starts to rise. The question now is: How high will your elephant fly? Figure 1: You and Your Elephant

THE APPROACH AND ASSUMPTIONS Using the Ideal Gas Law and Archimedes Principle you must first calculate the radius and volume of a spherical balloon filled with pure helium to a pressure of 101.3 kpa, that will just lift you, your elephant, the balloon bag. and the platform and harness. Assume your elephant weighs 4905 N, you weigh 490.5 N, the platform and harness weighs 490.5 N and the balloon bag weighs 0.981 N/meter squared. The sea level outside temperature is 288 K and the temperature of the helium is 288 K. Once you have designed your balloon in terms of determining its fixed radius and volume, you must determine how high the balloon will fly after you have been pushed off of the balloon. To do this we want you to use two approaches and compare them. In the first approach assume that the temperature of the atmosphere is constant and equal to 288K over the entire height from sea level (on the ground) to the final float height of the balloon after you are pushed off. In the second approach use the Properties of the U.S. Standard Atmosphere to determine the ratio of the air density at altitude to the air density at sea level with a sea level temperature of 288K. Assume that the volume of the balloon is fixed, and the material is strong enough to withstand the pressure difference between the inside and outside of the balloon as it rises to its final height. THE SOLUTION Determination of the Balloon Radius and Volume: To determine the volume of the balloon that will just lift you and your elephant at sea level we must calculate the buoyancy force, F B, and set it equal to the combined weights of the balloon, helium, harness and platform, girl and elephant. The buoyancy force, F B, is just equal to the weight of air, which the balloon displaces. Setting the buoyancy force equal to the weight of all the components, (equation 1), the radius and volume of the balloon are determined as shown below. In this calculation the volume of the girl and the elephant are neglected since they are small compared to the volume of the balloon. The weight of the displaced air and the weight of the helium in the balloon are determined from the Ideal Gas Law (equation 2). V = volume of balloon in cubic meters T = 288 K F B = W bag + W elephant + W girl +W harness +W helium Eq. 1 W bag = (surface area of balloon)(mass of balloon bag per sq meter)(g) = 4 (r 2 )(0.1)(9.81) = 12.33r 2 N W elephant = (m)(g) = (500)(9.81) = 4905 N.

RHe = gas constant for Helium, g = acceleration of gravity Ideal Gas Law Eq. 2 N Rair = gas constant for air N Force balance:, the volume of the spherical balloon Isothermal Calculation of How High the Elephant Flies: When the girl is pushed off of the balloon platform, the total weight is now reduced by 490.5 N and so the balloon rises until it reaches an altitude where the air density is lower and the new buoyancy force (equal to the new weight of displaced air) just balances the new total weight. When we make the assumption that the atmospheric temperature is constant and equal to 288K, then the density of the air as a function of altitude is given by equation 3 below. A derivation of this equation is presented in the appendix. The calculation is as follows: Isothermal Altitude Equation: Eq. 3, kilograms per cubic meter

, meters, kilograms per cubic meter Force balance: 0.9326 = ln.9326 = h / 8426 0.0698 = h / 8426 588 meters (1929 feet) is how high your elephant flies.

Calculation Using The U.S. Standard Atmosphere The 1976 U.S. Standard Atmosphere Tables 1 gives among other things the ratio of the air density at altitude to the air density at sea level. After the girl is pushed off of the balloon platform, the total weight of the balloon system is reduced by 490.5 N and the balloon rises to a higher float point where the buoyancy force just matches the new weight. As shown below the ratio of the density of air at the float point (without the girl) to the density of air at sea level is 0.932. Using the standard table the float point is 729 meters or 2392 feet. Total mass on ground with the girl: = 1.225 kg/meter cubed Total mass on the ground without the girl: Density at float point: kg/meter cubed Specific Gravity: From the Standard Altitude Table (reference 1), find h when density ratio is equal to 0.932 Comparison of Isothermal and Standard Atmosphere Assumptions With the isothermal assumption the float point was 1929 feet while the standard atmosphere calculation gave a value of 2392 feet. This is consistent with the fact that in the standard atmosphere tables the temperature drops with altitude, which results in the density at any given altitude being higher in the standard atmosphere case than in the isothermal case resulting in the float point being somewhat higher in the standard atmosphere case than in the isothermal case.

REFERENCE 1976 U.S Standard Atmosphere, www.digitaldutch.com/atmoscalc/ APPENDIX Derivation of Isothermal Altitude equation: Consider a column of air and a force balance around a differential element of the column (figure 2 below). The total force on the bottom of the differential element minus the force on the top of the differential element is just equal to the weight of air contained in the differential element. Let: P = pressure of air (kpa) at altitude, h P 0 = pressure of air at sea level R = specific gas constant (kj/kg/k) T = temperature (K) = air density (kg/meter cubed) at altitude, h o = air density at sea level (kg/meter cubed) A = area (meters squared) a = RT/g (meters) A(P- dp) AP = Agdh force balance around differential element of height (g=gravity consrant) Now, assume an isothermal atmosphere, where T and R are constants. =P/RT (ideal gas law) -dp= (P/RT)gdh dp = P 0 h dh = RT g g RT dh P Po dp P

h = RT g ln( P Po ) ln( P Po ) = gh RT h P Po = e a h h a a P = Poe and = oe Figure 2, Differential Element of a Column of Air