Calculating Pumpdown Times

Size: px
Start display at page:

Download "Calculating Pumpdown Times"

Transcription

1 Syllabus Changes 3/31/03 Outgassing and Permeation 4/7/03 Thin Film Deposition 4/14/03 Spring Break No Class 4/21/03 Field Trip to Semicore Equipment Corporation (coater manufacturer) 4//28/03 System Design Calculation Wrap-up Homework #3 Length 1 Length inches 4.9 inches conductance, liters/second Pbar (torr) C for 25 mm C for 50 mm 1.00E E E E E E E

2 Conductance Response 100 mm Angle Valve Conductance for two Gate-Seat Distances mm 50 mm Liters per Second E E E E-01 Pbar (Torr) Limitations of Equation 19! 15,800 l/s at 0.1 Torr! Velocity = Volume Flowrate/Area! Media Velocity is 2000 meters/sec!! Sonic Velocity is about 350 meters/s for sea level air. 2

3 Solution! Roth suggests using an implied sonic velocity of 192 meters/sec.! This is straightforward by introducing an aperture conductance in series with the pipe! Equation 29, where C is in l/s and A is given in square inches!c=130a Example Angle Valve Calculation conductance, liters/second Pbar (torr) 25 mm Aperture 25 & Aperture 1.00E E E E E E E Pbar (torr) 50 mm Aperture 50 & Aperture 1.00E E E E E E E

4 Response 100 mm Angle Valve Conductance for two Gate-Seat Distances mm 50 mm 25 & Aperture 50 & Aperture Liters per Second E E E E-01 Pbar (Torr) Comments! The error in the molecular conductance region would diminish if the angle valve had a real pipe connected to it.! Summary: Implement an aperture conductance in series when performing pumpdown calculations or if you suspect velocities are high. 4

5 Question: Consider a 100 liter Chamber with a 50 l/s exhaust system How many seconds does it take to evacuate the chamber? Answer The characteristic time constant of the system is 2 seconds. What pressure do you want to achieve? 5

6 What is a characteristic response time? Dissipative First order Systems Many physical process have a time dependent inclination to a restoring behavior which is dissipative in nature Take the equation Y=A/X where A is a constant Let s define Y to be Theta and X to be time, such that dθ = Kθdt dt 6

7 Rewriting and Integrating 1 dθ = Kdt θ lnθ = Kt + C Pressure and Temperature of Dissipative Systems We define theta as a nondimensional value that lives between zero and 1 and has a tendency towards zero For Pressure For Temperature θ = θ P Po P P max T P max T o 0 P o 7

8 Introducing Eq. 25. t = V S P ln 1 P 2 T=time (seconds) to pump from P 1 to P 2 V=Volume (liters) to be pumped S=delivered Pumping speed in liters/sec P 1 Starting pressure, torr P 2 Ending Pressure, torr Time constant of the system is V/S Y=A/X Y=1/X Y=5/X Y=25/x Y X 8

9 For Discussion: What is the meaning of the instantaneous time rate of change? What is the natural Log (Ln) of e? What is the natural Log of 1? What is the natural Log of 0 What is the difference between e and 10 logs? What is the area under the curve Y=1/X? Back to our pop quiz! V/S = 100/50 = 2 sec! When time = V/S, then Ln(P1/P2) = 1! And P2 is 36.78% of P1! We call this the characteristic time response. x e^x % % % % % % % 9

10 Limitations: "V/S has to be nearly constant. V is usually not a problem. The solution for S is to partition the problem where conductance changes are dramatic. Fortunately, this is easy to do in Excel. Pumpdown Example! 1 meter high by 50 cm dia. Cylindrical Vessel for a 40 mm foreline! 10 long 40 mm tubulation to an! Alcatel Dry Pump 122P operating in North America! Estimate Pumpdown time from Atmosphere to 0.01 Torr 10

11 Partitioning the Problem! Solution accuracy increased with greater number of steps! 7 steps are chosen here from 8 points taken from Manufacturers data! Be sure to employ equations using correct units (Torr, Inches, liters/sec) Relevant Equations are 20, 23, 24, 25 t V P ln = + + S C C S 1 = St P2 t aperture tube p C tube = 3000P D + 80D avg L 4 3 Caperture = 130A 11

12 Calculation using Excel P [Torr]Sp [liters/sec] Step# P avg S avg C tube C ap St V/St [sec] ln[p1/p2] Time [sec] Cum Time Pumpdown, sec 203 This excel datafile available for download and inspection in the Miscellaneous section of the class website. The Results Pumpdow n Time Pressure, Torr Time, seconds 12

13 Restrictions/Assumptions! System is leak tight! There are no internal gas loads. This assumption usually valid to 1.0E-02 Torr.! Humidity does play a role, and gases are assumed dry.! No safety factor included! Pumps perform to mfgr s specification! Gas is N2 equivalent Pumpdown A summary Pump usually limits behavior at atmosphere, unless pump is much larger than the tubulation. In this case aperture limits conductance. At lowest pressures, tubulation and pump (perhaps both) can dominate the pumpdown time. Results may not be accurate, but are nevertheless highly useful for system design 13

Physical Vapor Deposition

Physical Vapor Deposition Physical Vapor Deposition EVAPORATION SPUTTERING Typically used for metallization of semiconductors. Both Evaporation & Sputtering are done in vacuum environments. Typically: y Evaporation Pressures are

More information

VACUUM PUMPING METHODS

VACUUM PUMPING METHODS VACUUM PUMPING METHODS VACUUM PUMPS (METHODS) Positive Displacement Vacuum Gas Transfer Vacuum Kinetic Vacuum Entrapment Vacuum Adsorption Reciprocating Displacement Rotary Drag Fluid Entrainment Ion Transfer

More information

Vacuum. Residual pressure can thwart the best cryogenic design. Each gas molecule collision carries ~kt from the hot exterior to the cold interior.

Vacuum. Residual pressure can thwart the best cryogenic design. Each gas molecule collision carries ~kt from the hot exterior to the cold interior. Vacuum Residual pressure can thwart the best cryogenic design Each gas molecule collision carries ~kt from the hot exterior to the cold interior. 1 millitorr = 3.5x10¹³/cm³ Gas atoms leaving the hot surfaces

More information

Conductance of an aperture

Conductance of an aperture n Vacuum φ A 4 How many molecules travel through A in a time t? P P A onductance of an aperture 3 q φa 3.64 0 ( T / M) na Volume of gas passing through A? Q Q Q / ΔP 3.64 ( T / M ) 3 dv/dt q/n 3.64 0 (

More information

Lecture 4. Ultrahigh Vacuum Science and Technology

Lecture 4. Ultrahigh Vacuum Science and Technology Lecture 4 Ultrahigh Vacuum Science and Technology Why do we need UHV? 1 Atmosphere = 760 torr; 1 torr = 133 Pa; N ~ 2.5 10 19 molecules/cm 3 Hertz-Knudsen equation p ZW 1/ 2 ( 2mk T) At p = 10-6 Torr it

More information

Math 1A Test Fall 10 Show your work for credit. Write all responses on separate paper. Don t use a calculator.

Math 1A Test Fall 10 Show your work for credit. Write all responses on separate paper. Don t use a calculator. Math A - 3.7 Test Fall 0 Name Show your work for credit. Write all responses on separate paper. Don t use a calculator.. Open cylindrical tubes resonate at the approimate frequencies, f, where nv f = L+

More information

Lecture 10. Vacuum Technology and Plasmas Reading: Chapter 10. ECE Dr. Alan Doolittle

Lecture 10. Vacuum Technology and Plasmas Reading: Chapter 10. ECE Dr. Alan Doolittle Lecture 10 Vacuum Technology and Plasmas Reading: Chapter 10 Vacuum Science and Plasmas In order to understand deposition techniques such as evaporation, sputtering,, plasma processing, chemical vapor

More information

Conductance of an aperture

Conductance of an aperture n Vacuum φ 4 How many molecules travel through in a time t? P P onductance of an aperture q φ.64 0 ( T / M) n Volume of gas passing through? Q Q dv/dt q/n.64 0 ( T / M) Q P Q / ΔP.64 (T / M ) l/s.64 0

More information

Behavior of Three Types of Plasma Sources for Optical Coating

Behavior of Three Types of Plasma Sources for Optical Coating Behavior of Three Types of Plasma Sources for Optical Coating Ronald R. Willey Willey Optical, Consultants, 13039 Cedar Street, Charlevoix, MI 49720, USA Ph 231-237-9392, ron@willeyoptical.com ABSTRACT

More information

Dynamic Equipment and Process Simulation for Atomic Layer Deposition Technology

Dynamic Equipment and Process Simulation for Atomic Layer Deposition Technology Dynamic Equipment and Process Simulation for Atomic Layer Deposition Technology Wei Lei, Yuhong Cai, Laurent Henn-Lecordier and Gary W. Rubloff Department of Materials Science and Engineering and Institute

More information

Copyright 2008, University of Chicago, Department of Physics. Experiment I. RATIO OF SPECIFIC HEATS OF GASES; γ C p

Copyright 2008, University of Chicago, Department of Physics. Experiment I. RATIO OF SPECIFIC HEATS OF GASES; γ C p Experiment I RATIO OF SPECIFIC HEATS OF GASES; γ C p / C v 1. Recommended Reading M. W. Zemansky, Heat and Thermodynamics, Fifth Edition, McGraw Hill, 1968, p. 122-132, 161-2. 2. Introduction You have

More information

Vacuum Chambers. Type DK /DK /DK

Vacuum Chambers. Type DK /DK /DK Vacuum Chambers Type DK 020.010/DK 070.010/DK 050.010 Tel: (609) 924-3011 Fax (609) 924-3018 www.princetonscientific.com Email: info@princetonscientific.com Vacuum Chambers Application: Vacuum chambers

More information

Vacuum Pumps. Two general classes exist: Gas transfer physical removal of matter. Mechanical, diffusion, turbomolecular

Vacuum Pumps. Two general classes exist: Gas transfer physical removal of matter. Mechanical, diffusion, turbomolecular Vacuum Technology Vacuum Pumps Two general classes exist: Gas transfer physical removal of matter Mechanical, diffusion, turbomolecular Adsorption entrapment of matter Cryo, sublimation, ion Mechanical

More information

Practice Final Exam Solutions

Practice Final Exam Solutions Important Notice: To prepare for the final exam, study past exams and practice exams, and homeworks, quizzes, and worksheets, not just this practice final. A topic not being on the practice final does

More information

K n. III. Gas flow. 1. The nature of the gas : Knudsen s number. 2. Relative flow : Reynold s number R = ( dimensionless )

K n. III. Gas flow. 1. The nature of the gas : Knudsen s number. 2. Relative flow : Reynold s number R = ( dimensionless ) III. Gas flow. The nature of the gas : Knudsen s number K n λ d 2. Relative flow : U ρ d η U : stream velocity ρ : mass density Reynold s number R ( dimensionless ) 3. Flow regions - turbulent : R > 2200

More information

Non Newtonian Fluid Dynamics

Non Newtonian Fluid Dynamics PDHonline Course M417 (3 PDH) Non Newtonian Fluid Dynamics Instructor: Paul G. Conley, PE 2012 PDH Online PDH Center 5272 Meadow Estates Drive Fairfax, VA 22030-6658 Phone & Fax: 703-988-0088 www.pdhonline.org

More information

Heat Exchangers for Condensation and Evaporation Applications Operating in a Low Pressure Atmosphere

Heat Exchangers for Condensation and Evaporation Applications Operating in a Low Pressure Atmosphere Acta Polytechnica Vol. 52 No. 3/202 Heat Exchangers for Condensation and Evaporation Applications Operating in a Low Pressure Atmosphere Petr Kracík,JiříPospíšil, Ladislav Šnajdárek Brno University of

More information

MTH 230 COMMON FINAL EXAMINATION Fall 2005

MTH 230 COMMON FINAL EXAMINATION Fall 2005 MTH 230 COMMON FINAL EXAMINATION Fall 2005 YOUR NAME: INSTRUCTOR: INSTRUCTIONS 1. Print your name and your instructor s name on this page using capital letters. Print your name on each page of the exam.

More information

Practice Final Exam Solutions

Practice Final Exam Solutions Important Notice: To prepare for the final exam, one should study the past exams and practice midterms (and homeworks, quizzes, and worksheets), not just this practice final. A topic not being on the practice

More information

EXPERIMENT 1 Chemistry 110 LABORATORY SAFETY

EXPERIMENT 1 Chemistry 110 LABORATORY SAFETY EXPERIMENT 1 Chemistry 110 LABORATORY SAFETY MEASUREMENTS PURPOSE: The Purpose of this laboratory exercise is for the students to develop the skills of measuring length, volume, mass and temperature and

More information

New Test Results For Physical Separation Of Tritium From Noble Gases And It s Implications For Sensitivity And Accuracy In Air And Stack Monitoring

New Test Results For Physical Separation Of Tritium From Noble Gases And It s Implications For Sensitivity And Accuracy In Air And Stack Monitoring New Test Results For Physical Separation Of Tritium From Noble Gases And It s Implications For Sensitivity And Accuracy In Air And Stack Monitoring -Robert Goldstein, Ivan Mitev, Dell Williamson, Overhoff

More information

Energy loss of alpha particles - Prelab questions

Energy loss of alpha particles - Prelab questions Energy loss of alpha particles - Prelab questions 1. Write down the decay path from 226 Ra to 206 Pb. Show the intermediate nuclides and the nuclear reactions which cause each transformation (α/β ± decay).

More information

EF 152 Exam 1 Spring 2018 Version 1 Page 1 Copy 640

EF 152 Exam 1 Spring 2018 Version 1 Page 1 Copy 640 EF 152 Exam 1 Spring 2018 Version 1 Page 1 Copy 640 Name: Seat Assignment: Specify your EXAM ID on the right. Use 000 if you don t know your exam ID. Circle your TEAM SECTION 0 0 0 1 1 1 102 216 217 218

More information

Section K MATH 211 Homework Due Friday, 8/30/96 Professor J. Beachy Average: 15.1 / 20. ), and f(a + 1).

Section K MATH 211 Homework Due Friday, 8/30/96 Professor J. Beachy Average: 15.1 / 20. ), and f(a + 1). Section K MATH 211 Homework Due Friday, 8/30/96 Professor J. Beachy Average: 15.1 / 20 # 18, page 18: If f(x) = x2 x 2 1, find f( 1 2 ), f( 1 2 ), and f(a + 1). # 22, page 18: When a solution of acetylcholine

More information

( ) ( ). ( ) " d#. ( ) " cos (%) " d%

( ) ( ). ( )  d#. ( )  cos (%)  d% Math 22 Fall 2008 Solutions to Homework #6 Problems from Pages 404-407 (Section 76) 6 We will use the technique of Separation of Variables to solve the differential equation: dy d" = ey # sin 2 (") y #

More information

Study fluid dynamics. Understanding Bernoulli s Equation.

Study fluid dynamics. Understanding Bernoulli s Equation. Chapter Objectives Study fluid dynamics. Understanding Bernoulli s Equation. Chapter Outline 1. Fluid Flow. Bernoulli s Equation 3. Viscosity and Turbulence 1. Fluid Flow An ideal fluid is a fluid that

More information

Differential Equations: Homework 8

Differential Equations: Homework 8 Differential Equations: Homework 8 Alvin Lin January 08 - May 08 Section.6 Exercise Find a general solution to the differential equation using the method of variation of parameters. y + y = tan(t) r +

More information

Vacuum and mechanical design of ILC DR

Vacuum and mechanical design of ILC DR Vacuum and mechanical design of ILC DR O. B. Malyshev ASTeC Vacuum Science Group, STFC Daresbury Laboratory, UK Low Emittance Ring Workshop 2010 12-15 January 2010 Integration design: usual consideration

More information

9. Pumps (compressors & turbines) Partly based on Chapter 10 of the De Nevers textbook.

9. Pumps (compressors & turbines) Partly based on Chapter 10 of the De Nevers textbook. Lecture Notes CHE 31 Fluid Mechanics (Fall 010) 9. Pumps (compressors & turbines) Partly based on Chapter 10 of the De Nevers textbook. Basics (pressure head, efficiency, working point, stability) Pumps

More information

Math 147 Exam II Practice Problems

Math 147 Exam II Practice Problems Math 147 Exam II Practice Problems This review should not be used as your sole source for preparation for the exam. You should also re-work all examples given in lecture, all homework problems, all lab

More information

CapaciTorr HV Pumps. making innovation happen,together

CapaciTorr HV Pumps. making innovation happen,together CapaciTorr HV Pumps making innovation happen,together CapaciTorr HV HIGHLIGHTS General Features High pumping speed for all active gases High sorption capacity and increased lifetime Constant pumping speed

More information

CapaciTorr HV 200 HIGHLIGHTS

CapaciTorr HV 200 HIGHLIGHTS CapaciTorr HV 200 General Features High pumping speed for all active gases High sorption capacity and increased lifetime Costant pumping speed in HV, UHV and XHV Reversible pumping of hydrogen and its

More information

( )dt F. ( ) = y 2 sin y. ( ) = t 2 sint dt. ( ) = 1+ 2x. ( ) = 1+ 2t dt. ( ) = cos t 2. ( ) = cos x 2 ( ) ( ) = arctan 1 x 1 x 2 = 1 x 2 arctan 1 x

( )dt F. ( ) = y 2 sin y. ( ) = t 2 sint dt. ( ) = 1+ 2x. ( ) = 1+ 2t dt. ( ) = cos t 2. ( ) = cos x 2 ( ) ( ) = arctan 1 x 1 x 2 = 1 x 2 arctan 1 x Section. The Fndamental Theorem of Calcls Part Soltions. g y g y y ( ) t sint dt ( ) y sin y. g g ( ) + t dt ( ) +. F ( )dt ( ) cos t F ( )dt F ( ) cos t ( ) ( ) cos. h ( ) arctant dt ( ) arctan arctan

More information

John Chubb Infostatic, 2 Monica Drive, Pittville, Cheltenham, GL50 4NQ, UK Website:

John Chubb Infostatic, 2 Monica Drive, Pittville, Cheltenham, GL50 4NQ, UK   Website: AN ALTERNATIVE APPROACH FOR CHARGE DECAY MEASUREMENT TO ASSESS THE SUITABILITY OF MATERIALS John Chubb Infostatic, 2 Monica Drive, Pittville, Cheltenham, GL50 4NQ, UK email: jchubb@infostatic.co.uk Website:

More information

Arc Length and Surface Area in Parametric Equations

Arc Length and Surface Area in Parametric Equations Arc Length and Surface Area in Parametric Equations MATH 211, Calculus II J. Robert Buchanan Department of Mathematics Spring 2011 Background We have developed definite integral formulas for arc length

More information

Pumping Speed in the Drydown Zone

Pumping Speed in the Drydown Zone A Journal of Practical and Useful Vacuum Technology From By Phil Danielson Pumping Speed in the Drydown Zone The extended pumpdown time through the water vapor-dominated drydown zone is a complex process

More information

BE SURE THAT YOU HAVE LOOKED AT, THOUGHT ABOUT AND TRIED THE SUGGESTED PROBLEMS ON THIS REVIEW GUIDE PRIOR TO LOOKING AT THESE COMMENTS!!!

BE SURE THAT YOU HAVE LOOKED AT, THOUGHT ABOUT AND TRIED THE SUGGESTED PROBLEMS ON THIS REVIEW GUIDE PRIOR TO LOOKING AT THESE COMMENTS!!! Review Guide for MAT0 Final Eam Part I. Thursday December 7 th during regular class time Part is worth 50% of your Final Eam grade. Syllabus approved calculators can be used on this part of the eam but

More information

Explosion Properties of Highly Concentrated Ozone Gas. 1 Iwatani International Corporation, Katsube, Moriyama, Shiga , Japan

Explosion Properties of Highly Concentrated Ozone Gas. 1 Iwatani International Corporation, Katsube, Moriyama, Shiga , Japan Explosion Properties of Highly Concentrated Ozone Gas Kunihiko Koike 1*, Masaharu Nifuku 2, Koichi Izumi 1, Sadaki Nakamura 1, Shuzo Fujiwara 2 and Sadashige Horiguchi 2 1 Iwatani International Corporation,

More information

Making Decisions with Insulation

Making Decisions with Insulation More on Heat Transfer from Cheresources.com: FREE Resources Making Decisions with Insulation Article: Basics of Vaporization Questions and Answers: Heat Transfer Experienced-Based Rules for Heat Exchangers

More information

Basic Theory of Differential Equations

Basic Theory of Differential Equations page 104 104 CHAPTER 1 First-Order Differential Equations 16. The following initial-value problem arises in the analysis of a cable suspended between two fixed points y = 1 a 1 + (y ) 2, y(0) = a, y (0)

More information

A STUDY OF RADON ADSORPTION ON ACTIVATED CARBON AS A FUNCTION OF TEMPERATURE

A STUDY OF RADON ADSORPTION ON ACTIVATED CARBON AS A FUNCTION OF TEMPERATURE A STUDY OF RADON ADSORPTION ON ACTIVATED CARBON AS A FUNCTION OF TEMPERATURE Stephen I. Shefsky, Daniel Rose, and Charles G. Parsons NITON Corporation Bedford, MA ABSTRACT The adsorption of radon-222 on

More information

NEXTorr HV 100 HIGHLIGHTS

NEXTorr HV 100 HIGHLIGHTS NEXTorr HV 100 HIGHLIGHTS General Features High pumping speed for all active gases Pumping speed for noble gases and methane High sorption capacity and increased lifetime Constant pumping speed in HV and

More information

AE 3051, Lab #16. Investigation of the Ideal Gas State Equation. By: George P. Burdell. Group E3

AE 3051, Lab #16. Investigation of the Ideal Gas State Equation. By: George P. Burdell. Group E3 AE 3051, Lab #16 Investigation of the Ideal Gas State Equation By: George P. Burdell Group E3 Summer Semester 000 Abstract The validity of the ideal gas equation of state was experimentally tested for

More information

Physics 4C Spring 2017 Test 1

Physics 4C Spring 2017 Test 1 Physics 4C Spring 017 Test 1 Name: April 19, 017 Please show your work! Answers are not complete without clear reasoning. When asked for an expression, you must give your answer in terms of the variables

More information

The Kestrel Handheld Weather Tracker. 1) If the unit is configured to log data and it is turned off, will it continue to log temperature data?

The Kestrel Handheld Weather Tracker. 1) If the unit is configured to log data and it is turned off, will it continue to log temperature data? The Kestrel Handheld Weather Tracker 1) If the unit is configured to log data and it is turned off, will it continue to log temperature data? Wind data? 2) If you turn on the unit and it doesn t take you

More information

Updating the International Standard Classification of Occupations (ISCO) Draft ISCO-08 Group Definitions: Occupations in Chemicals

Updating the International Standard Classification of Occupations (ISCO) Draft ISCO-08 Group Definitions: Occupations in Chemicals International Labour Organization Organisation internationale du Travail Organización Internacional del Trabajo Updating the International Standard Classification of Occupations (ISCO) Draft ISCO-08 Group

More information

Safety Engineering. -Static Electricity and Charge Accumulation-

Safety Engineering. -Static Electricity and Charge Accumulation- Safety Engineering -Static Electricity and Charge Accumulation- Definitions - Types of materials 2 Conductive A material with a low electrical resistance, electrons flow easily across the surface or through

More information

Vacuum I. G. Franchetti CAS - Bilbao. 30/5/2011 G. Franchetti 1

Vacuum I. G. Franchetti CAS - Bilbao. 30/5/2011 G. Franchetti 1 Vacuum I G. Franchetti CAS - Bilbao 30/5/2011 G. Franchetti 1 Index Introduction to Vacuum Vacuum and the Beam Flow Regimes Creating Vacuum 30/5/2011 G. Franchetti 2 Vacuum in accelerators All beam dynamics

More information

The final is comprehensive (8-9 pages). There will be two pages on ch 9.

The final is comprehensive (8-9 pages). There will be two pages on ch 9. Closing Wed: HW_9A,9B (9.3/4,3.8) Final: Sat, Dec. 9 th, 1:30-4:20, KANE 130 Assigned seats, for your seat go to: catalyst.uw.edu/gradebook/aloveles/102715 The final is comprehensive (8-9 pages). There

More information

ME 309 Fluid Mechanics Fall 2010 Exam 2 1A. 1B.

ME 309 Fluid Mechanics Fall 2010 Exam 2 1A. 1B. Fall 010 Exam 1A. 1B. Fall 010 Exam 1C. Water is flowing through a 180º bend. The inner and outer radii of the bend are 0.75 and 1.5 m, respectively. The velocity profile is approximated as C/r where C

More information

EXPERIMENT 3. HEAT-CAPACITY RATIOS FOR GASES

EXPERIMENT 3. HEAT-CAPACITY RATIOS FOR GASES EXERIMENT 3. HEAT-CAACITY RATIOS FOR GASES The ratio Cp/Cv of the heat capacity of a gas at constant pressure to that at constant volume will be determined by either the method of adiabatic expansion.

More information

Nicholas J. Giordano. Chapter 10 Fluids

Nicholas J. Giordano.  Chapter 10 Fluids Nicholas J. Giordano www.cengage.com/physics/giordano Chapter 10 Fluids Fluids A fluid may be either a liquid or a gas Some characteristics of a fluid Flows from one place to another Shape varies according

More information

Homework 01. Phase Changes and Solutions

Homework 01. Phase Changes and Solutions HW01 - Phase Changes and Solu!ons! This is a preview of the published version of the quiz Started: Jan 16 at 1:pm Quiz Instruc!ons Homework 01 Phase Changes and Solutions Question 1 Given that you have

More information

10 March Conductance/Microscopes/MFC s. Flow Characteristics can be reduced to a function of pipe diameter and pressure. Las Positas College

10 March Conductance/Microscopes/MFC s. Flow Characteristics can be reduced to a function of pipe diameter and pressure. Las Positas College 10 March 2003!More Isolation Applications!Conductance in!mitered Elbows!Radiused Elbows!MFC s and Gas Sources!Vacuum Microscopes Flow Characteristics can be reduced to a function of pipe diameter and pressure

More information

Lab #4 Similitude: The Kármán Vortex Street CEE 331 Fall 2004

Lab #4 Similitude: The Kármán Vortex Street CEE 331 Fall 2004 CEE 331 Lab 4 Page 1 of 6 Lab #4 Similitude: The Kármán Vortex Street CEE 331 Fall 2004 Safety The major safety hazard in this laboratory is a shock hazard. Given that you will be working with water and

More information

EF 152 Final Exam Fall 2018 Page 1 Copy 160

EF 152 Final Exam Fall 2018 Page 1 Copy 160 EF 152 Final Exam Fall 2018 Page 1 Copy 160 Name: Seat Assignment: Specify your EXAM ID on the right. Use 000 if you don t know your exam ID. Circle your TEAM SECTION 11:10 12:40 2:10 216 217 218 A216

More information

Practice Exam 1 Solutions

Practice Exam 1 Solutions Practice Exam 1 Solutions 1a. Let S be the region bounded by y = x 3, y = 1, and x. Find the area of S. What is the volume of the solid obtained by rotating S about the line y = 1? Area A = Volume 1 1

More information

AP Physics C: Work, Energy, and Power Practice

AP Physics C: Work, Energy, and Power Practice AP Physics C: Work, Energy, and Power Practice 1981M2. A swing seat of mass M is connected to a fixed point P by a massless cord of length L. A child also of mass M sits on the seat and begins to swing

More information

MAC 2311 Calculus I Spring 2004

MAC 2311 Calculus I Spring 2004 MAC 2 Calculus I Spring 2004 Homework # Some Solutions.#. Since f (x) = d dx (ln x) =, the linearization at a = is x L(x) = f() + f ()(x ) = ln + (x ) = x. The answer is L(x) = x..#4. Since e 0 =, and

More information

YOUR HW MUST BE STAPLED YOU MUST USE A PENCIL (no pens)

YOUR HW MUST BE STAPLED YOU MUST USE A PENCIL (no pens) Spring 2008 CIVE 462 HOMEWORK #1 1. Print out the syllabus. Read it. Write the grade percentages in the first page of your notes. 2. Go back to your 301 notes, internet, etc. and find the engineering definition

More information

MATH 152, Fall 2017 COMMON EXAM II - VERSION A

MATH 152, Fall 2017 COMMON EXAM II - VERSION A MATH 15, Fall 17 COMMON EXAM II - VERSION A LAST NAME(print): FIRST NAME(print): INSTRUCTOR: SECTION NUMBER: DIRECTIONS: 1. The use of a calculator, laptop or computer is prohibited.. TURN OFF cell phones

More information

Calculus II Practice Test Problems for Chapter 7 Page 1 of 6

Calculus II Practice Test Problems for Chapter 7 Page 1 of 6 Calculus II Practice Test Problems for Chapter 7 Page of 6 This is a set of practice test problems for Chapter 7. This is in no way an inclusive set of problems there can be other types of problems on

More information

10.52 Mechanics of Fluids Spring 2006 Problem Set 3

10.52 Mechanics of Fluids Spring 2006 Problem Set 3 10.52 Mechanics of Fluids Spring 2006 Problem Set 3 Problem 1 Mass transfer studies involving the transport of a solute from a gas to a liquid often involve the use of a laminar jet of liquid. The situation

More information

MAS113 CALCULUS II SPRING 2008, QUIZ 5 SOLUTIONS. x 2 dx = 3y + y 3 = x 3 + c. It can be easily verified that the differential equation is exact, as

MAS113 CALCULUS II SPRING 2008, QUIZ 5 SOLUTIONS. x 2 dx = 3y + y 3 = x 3 + c. It can be easily verified that the differential equation is exact, as MAS113 CALCULUS II SPRING 008, QUIZ 5 SOLUTIONS Quiz 5a Solutions (1) Solve the differential equation y = x 1 + y. (1 + y )y = x = (1 + y ) = x = 3y + y 3 = x 3 + c. () Solve the differential equation

More information

SCM Series Supercapacitor Modules Series-Connected Supercapacitors

SCM Series Supercapacitor Modules Series-Connected Supercapacitors The new series of cylindrical electrochemical double-layer capacitors offers excellent pulse power handling characteristics based on the combination of very high capacitance and very low. Used by themselves

More information

Mass Spectrometry for Equipment, Process and Wafer State Sensing and Control

Mass Spectrometry for Equipment, Process and Wafer State Sensing and Control Mass Spectrometry for Equipment, Process and Wafer State Sensing and Control Laura L. Tedder, G. Brian Lu and Gary W. Rubloff laura_tedder@ucsd.edu brian_lu@ncsu.edu gary_rubloff@ncsu.edu NSF Engineering

More information

PHY321 Homework Set 2

PHY321 Homework Set 2 PHY321 Homework Set 2 1. [5 pts] Consider the forces from the previous homework set, F A ( r )and F B ( r ), acting on a particle. The force components depend on position r of the particle according to

More information

C ONTENTS CHAPTER TWO HEAT CONDUCTION EQUATION 61 CHAPTER ONE BASICS OF HEAT TRANSFER 1 CHAPTER THREE STEADY HEAT CONDUCTION 127

C ONTENTS CHAPTER TWO HEAT CONDUCTION EQUATION 61 CHAPTER ONE BASICS OF HEAT TRANSFER 1 CHAPTER THREE STEADY HEAT CONDUCTION 127 C ONTENTS Preface xviii Nomenclature xxvi CHAPTER ONE BASICS OF HEAT TRANSFER 1 1-1 Thermodynamics and Heat Transfer 2 Application Areas of Heat Transfer 3 Historical Background 3 1-2 Engineering Heat

More information

Anomalous production of gaseous 4 He at the inside of DScathode during D 2 O-electrolysis

Anomalous production of gaseous 4 He at the inside of DScathode during D 2 O-electrolysis Arata, Y. and Y.C. Zhang, Anomalous production of gaseous 4 He at the inside of 'DS cathode' during D 2 O- electrolysis. Proc. Jpn. Acad., Ser. B, 1999. 75: p. 281. Anomalous production of gaseous 4 He

More information

MAHATMA GANDHI MISSION S JAWAHARLAL NEHRU ENGINEERING COLLEGE, FLUID MECHANICS LABORATORY MANUAL

MAHATMA GANDHI MISSION S JAWAHARLAL NEHRU ENGINEERING COLLEGE, FLUID MECHANICS LABORATORY MANUAL MAHATMA GANDHI MISSION S JAWAHARLAL NEHRU ENGINEERING COLLEGE, AURANGABAD. (M.S.) DEPARTMENT OF CIVIL ENGINEERING FLUID MECHANICS LABORATORY MANUAL Prepared By Mr. L. K. Kokate Lab Incharge Approved By

More information

Speed Distribution at CONSTANT Temperature is given by the Maxwell Boltzmann Speed Distribution

Speed Distribution at CONSTANT Temperature is given by the Maxwell Boltzmann Speed Distribution Temperature ~ Average KE of each particle Particles have different speeds Gas Particles are in constant RANDOM motion Average KE of each particle is: 3/2 kt Pressure is due to momentum transfer Speed Distribution

More information

1/54 Circulation pump, safety valve, expansion vessel

1/54 Circulation pump, safety valve, expansion vessel 1/54 Circulation pump, safety valve, expansion vessel pressure loss efficiency of pump secured heat output safety valve sizing expansion vessel sizing Circulation pump 2/54 similar principle as for heating

More information

!! +! 2!! +!"!! =!! +! 2!! +!"!! +!!"!"!"

!! +! 2!! +!!! =!! +! 2!! +!!! +!!!! Homework 4 Solutions 1. (15 points) Bernoulli s equation can be adapted for use in evaluating unsteady flow conditions, such as those encountered during start- up processes. For example, consider the large

More information

Applied Calculus I Practice Final Exam Solution Notes

Applied Calculus I Practice Final Exam Solution Notes AMS 5 (Fall, 2009). Solve for x: 0 3 2x = 3 (.2) x Taking the natural log of both sides, we get Applied Calculus I Practice Final Exam Solution Notes Joe Mitchell ln 0 + 2xln 3 = ln 3 + xln.2 x(2ln 3 ln.2)

More information

University of Toronto Solutions to MAT187H1S TERM TEST of Thursday, March 20, 2008 Duration: 90 minutes

University of Toronto Solutions to MAT187H1S TERM TEST of Thursday, March 20, 2008 Duration: 90 minutes University of Toronto Solutions to MAT187H1S TERM TEST of Thursday, March 2, 28 Duration: 9 minutes Only aids permitted: Casio 26, Sharp 52, or Texas Instrument 3 calculator. Instructions: Make sure this

More information

Exercise 4-3. Titration of Weak Acids EXERCISE OBJECTIVE DISCUSSION OUTLINE. The 5% rule DISCUSSION

Exercise 4-3. Titration of Weak Acids EXERCISE OBJECTIVE DISCUSSION OUTLINE. The 5% rule DISCUSSION Exercise 4-3 Titration of Weak Acids EXERCISE OBJECTIVE Titrate both a weak acid solution and a weak polyprotic acid solution with a strong base solution. Plot a graph using the titration data, analyze

More information

a. 4.2x10-4 m 3 b. 5.5x10-4 m 3 c. 1.2x10-4 m 3 d. 1.4x10-5 m 3 e. 8.8x10-5 m 3

a. 4.2x10-4 m 3 b. 5.5x10-4 m 3 c. 1.2x10-4 m 3 d. 1.4x10-5 m 3 e. 8.8x10-5 m 3 The following two problems refer to this situation: #1 A cylindrical chamber containing an ideal diatomic gas is sealed by a movable piston with cross-sectional area A = 0.0015 m 2. The volume of the chamber

More information

Commenting template CEN/TC 102 Date : Document: pren 13060

Commenting template CEN/TC 102 Date : Document: pren 13060 Commenting template CEN/TC 0 Date : 006-09-3 Document: pren 3060 MB Clause / 3.) ) FR general Ge There have been so many discussions during the CEN/TC 0/WG5 meetings these years. The committee has recognised

More information

UHV - Technology. Oswald Gröbner

UHV - Technology. Oswald Gröbner School on Synchrotron Radiation UHV - Technology Trieste, 20-21 April 2004 1) Introduction and some basics 2) Building blocks of a vacuum system 3) How to get clean ultra high vacuum 4) Desorption phenomena

More information

I. INTRODUCTION AND LABORATORY SAFETY

I. INTRODUCTION AND LABORATORY SAFETY EXPERIMENT 1 Chemistry 100 Measurement Techniques and Safety Purpose: To Learn the basic techniques of laboratory measurement of mass, temperature, volume and length and the concepts of safety I. INTRODUCTION

More information

Note: Unless otherwise specified, the domain of a function f is assumed to be the set of all real numbers x for which f (x) is a real number.

Note: Unless otherwise specified, the domain of a function f is assumed to be the set of all real numbers x for which f (x) is a real number. 997 AP Calculus BC: Section I, Part A 5 Minutes No Calculator Note: Unless otherwise specified, the domain of a function f is assumed to be the set of all real numbers for which f () is a real number..

More information

Math Exam 02 Review

Math Exam 02 Review Math 10350 Exam 02 Review 1. A differentiable function g(t) is such that g(2) = 2, g (2) = 1, g (2) = 1/2. (a) If p(t) = g(t)e t2 find p (2) and p (2). (Ans: p (2) = 7e 4 ; p (2) = 28.5e 4 ) (b) If f(t)

More information

All work must be shown in this course for full credit. Unsupported answers may receive NO credit.

All work must be shown in this course for full credit. Unsupported answers may receive NO credit. AP Calculus 6.. Worksheet Estimating with Finite Sums All work must be shown in this course for full credit. Unsupported answers may receive NO credit.. Suppose an oil pump is producing 8 gallons per hour

More information

Calculation of Pipe Friction Loss

Calculation of Pipe Friction Loss Doc.No. 6122-F3T071 rev.2 Calculation of Pipe Friction Loss Engineering Management Group Development Planning Department Standard Pump Business Division EBARA corporation October 16th, 2013 1 / 33 2 /

More information

Review for Chapter 8

Review for Chapter 8 Review for Chapter 8 The function v(t) is the velocity of an object moving on the x-axis at any time t 0 where the velocity is measured in ft/sec. a) Determine when the object is moving right, left and

More information

Photosynthesis. Lab Exercise 9. Contents. Introduction. Objectives

Photosynthesis. Lab Exercise 9. Contents. Introduction. Objectives Lab Exercise Photosynthesis Contents Objectives 1 Introduction 1 Activity.1 Action Spectrum 2 Activity.2 Effects of Temperature 4 Activity.3 Photosynthesis Experiment 4 Resutls Section 5 Objectives - Quantify

More information

Mathematical Modeling Project in Mathematica Cynthia Wenz MA 354

Mathematical Modeling Project in Mathematica Cynthia Wenz MA 354 clw.ma 1 Mathematical Modeling Project in Mathematica Cynthia Wenz MA 354 Introduction and Problem Statement When a parachute jump is made from an airplane, the first part of the descent is made in free

More information

Quiz 4A Solutions. Math 150 (62493) Spring Name: Instructor: C. Panza

Quiz 4A Solutions. Math 150 (62493) Spring Name: Instructor: C. Panza Math 150 (62493) Spring 2019 Quiz 4A Solutions Instructor: C. Panza Quiz 4A Solutions: (20 points) Neatly show your work in the space provided, clearly mark and label your answers. Show proper equality,

More information

All work must be shown in this course for full credit. Unsupported answers may receive NO credit.

All work must be shown in this course for full credit. Unsupported answers may receive NO credit. AP Calculus 5. Worksheet All work must be shown in this course for full credit. Unsupported answers may receive NO credit.. Suppose an oil pump is producing 8 gallons per hour for the first 5 hours of

More information

Preparations for proof-of- principle D-T IEC experiments

Preparations for proof-of- principle D-T IEC experiments 14 th US-Japan Workshop on IEC October 15-16, 2012 University of Maryland Preparations for proof-of- principle D-T IEC experiments Yasushi YAMAMOTO 1, Masami Ohnishi 1, Hodaka, Osawa 1, Yuji Hatano 2 and

More information

Lecture 5. Labs this week:

Lecture 5. Labs this week: Labs this week: Lab 10: Bleed-off Circuit Lecture 5 Lab 11/12: Asynchronous/Synchronous and Parallel/Tandem Operations Systems Review Homework (due 10/11) Participation is research lab Hydraulic Hybrid

More information

3.1 Definitions States of Matter

3.1 Definitions States of Matter 3.1 Definitions States of Matter WORDS FOR DEFINITIONS YOU NEED ARE IN RED Phase /state Solid Liquid Gas Elastic Collision Kinetic Theory Volume Pressure Temperature Absolute Zero Temp Celsius Kelvin Fahrenheit

More information

Math 116 Second Midterm March 20, 2013

Math 116 Second Midterm March 20, 2013 Math 6 Second Mierm March, 3 Name: EXAM SOLUTIONS Instructor: Section:. Do not open this exam until you are told to do so.. This exam has 3 pages including this cover. There are 8 problems. Note that the

More information

Exercise 5-1. Water Deionization EXERCISE OBJECTIVE DISCUSSION OUTLINE. Introduction DISCUSSION. An ions story

Exercise 5-1. Water Deionization EXERCISE OBJECTIVE DISCUSSION OUTLINE. Introduction DISCUSSION. An ions story Exercise 5-1 Water Deionization EXERCISE OBJECTIVE Familiarize yourself with conductivity probes and learn how to calibrate and use them for conductivity measurement. Also, learn how ion-exchange resins

More information

Lagrangian description from the perspective of a parcel moving within the flow. Streamline Eulerian, tangent line to instantaneous velocity field.

Lagrangian description from the perspective of a parcel moving within the flow. Streamline Eulerian, tangent line to instantaneous velocity field. Chapter 2 Hydrostatics 2.1 Review Eulerian description from the perspective of fixed points within a reference frame. Lagrangian description from the perspective of a parcel moving within the flow. Streamline

More information

INSTITUTE OF AERONAUTICAL ENGINEERING Dundigal, Hyderabad AERONAUTICAL ENGINEERING QUESTION BANK : AERONAUTICAL ENGINEERING.

INSTITUTE OF AERONAUTICAL ENGINEERING Dundigal, Hyderabad AERONAUTICAL ENGINEERING QUESTION BANK : AERONAUTICAL ENGINEERING. Course Name Course Code Class Branch INSTITUTE OF AERONAUTICAL ENGINEERING Dundigal, Hyderabad - 00 0 AERONAUTICAL ENGINEERING : Mechanics of Fluids : A00 : II-I- B. Tech Year : 0 0 Course Coordinator

More information

Experimental and Theoretical Evaluation of the Overall Heat Loss Coefficient of a Vacuum Tube Solar Collector

Experimental and Theoretical Evaluation of the Overall Heat Loss Coefficient of a Vacuum Tube Solar Collector Experimental and Theoretical Evaluation of the Overall Heat Loss Coefficient of a Vacuum Tube Solar Collector Abdul Waheed Badar *, Reiner Buchholz, and Felix Ziegler Institut für Energietechnik, KT, FG

More information

EXPERIMENTAL AND NUMERICAL STUDIES OF A SPIRAL PLATE HEAT EXCHANGER

EXPERIMENTAL AND NUMERICAL STUDIES OF A SPIRAL PLATE HEAT EXCHANGER THERMAL SCIENCE: Year 2014, Vol. 18, No. 4, pp. 1355-1360 1355 EXPERIMENTAL AND NUMERICAL STUDIES OF A SPIRAL PLATE HEAT EXCHANGER by Rangasamy RAJAVEL Department of Mechanical Engineering, AMET University,

More information

Model Selection 1. Process Valves. Air. Vacuum

Model Selection 1. Process Valves. Air. Vacuum Process Valves Model Selection For product specifications such as maximum operating pressure differentials and operating temperature ranges, refer to the relevent pages of each product. Air One-touch fittings

More information

1.060 Engineering Mechanics II Spring Problem Set 2

1.060 Engineering Mechanics II Spring Problem Set 2 1.060 Engineering Mechanics II Spring 2006 Due on Monday, February 27th Problem Set 2 Important note: Please start a new sheet of paper for each problem in the problem set. Write the names of the group

More information