Progress Report Yu ZHANG Directed by Prof. Wen J. LI July 2, 2010.

Slides:



Advertisements
Similar presentations
ISENTROPIC EFFICIENCY CALCULATIONS POSITIVE-DISPLACEMENT
Advertisements

Air Stripping (Section 9 – 1)
Mechanical Waves Types of Wave Describing Waves The Wave Equation.
Advanced Thermodynamics Note 6 Applications of Thermodynamics to Flow Processes Lecturer: 郭修伯.
Lecture 2 Buoyancy. Fluid dynamics. Hot air balloon Buoyancy (in the Dead Sea) Cohesion (water bubble in space) Laminar flow.
Ch 3.8: Mechanical & Electrical Vibrations
CHE-201: Introduction to Chemical Engineering
A Macroscopic Description of Matter (Phase Changes & Ideal Gases)
Chapter 2: Overall Heat Transfer Coefficient
Laws of Thermodynamics The first law states that the change in the energy of a system is the amount of energy added to the system minus the energy spent.
Long Term Storage Long term storage means to store water during high inflows years for the benefit of low inflows years. Long term storage means to store.
CHE Overall Energy Balance Overall Energy Balance Objectives 1.To be able to derive overall energy balance from the 1 st law of thermodynamics 2.To.
Spiral Condensors. Working Principle The Spiral Condensor consists of two sheets stainless steel strips which have been wounded from the centre.
Fluid Flow and Continuity Imagine that a fluid flows with a speed v 1 through a cylindrical pip of cross-sectional area A 1. If the pipe narrows to a cross-
Using the Ideal Gas Law and Previously Learned Concepts
CHE 205 $200 $400 $600 $800 $1000 Vapor/Liquid Equilibrium Energy Balances Multiphase Systems Nonreactive Processes $600.
Pressure in Fluid Systems
Upscaling of Foam Mobility Control to Three Dimensions Busheng Li George Hirasaki Clarence Miller Rice University, Houston, TX.
2nd Law of Thermodynamics 1st Law: energy is conserved But is that enough ? –Object drops converting KE to heat but never see the opposite –H 2 and O 2.
G. Monni, M. De Salve, B. Panella Politecnico di Torino, C.so Duca degli Abruzzi 24, Torino HEFAT th International.
Standard Molar Enthalpies of Formation ΔHfoΔHfo. Focus Questions 1) What are formation reactions? 2) What is standard molar enthalpy of formation? 3)
Partial Pressure Problems. Vocabulary Used in Partial Pressure Problems 1. Partial Pressure- The pressure of each gas in a mixture. 2. Dalton’s Law- The.
1.What is ‘α’ called? 2.What is ‘β’ called? 3.Define the term ‘refraction’ 4.α = 42 o, β = 30 o, v 1 = 7ms -1 and λ 1 = 2m. Using Snell’s law, calculate:
BUOYANT FORCE LESSON 2. Buoyant Forces and Liquid Buoyant Force is an upward force which acts on an object that is being completely or partially immersed.
DIFFERENTIAL MANOMETER
Lesson 13 Gases and Vapors Anything in black letters = write it in your notes (‘knowts’)
Dimensional analysis Drag force on sphere depends on: The velocity U
Dalton’s Law of Partial Pressure  John Dalton responsible for atomic theory responsible for atomic theory also studied gas mixtures also studied gas.
Mechanics Exercise Class Ⅳ
Inputs/Givens 1.Volume of Ice (3.5 gal) 2.Density of Ice (736 kg/m 3 ) 3.Latent Heat of Ice, h sf (333.6 KJ/kg) 4.Melt time of 1 hour (3600 s) Constraints.
1 Thermodynamics The study of energy conversions between heat and other forms.
13 Oct 2011Prof. R. Shanthini1 Course content of Mass transfer section LTA Diffusion Theory of interface mass transfer Mass transfer coefficients, overall.
Introduction to Fluid Mechanics Engineering 1h Prof Bill Easson.
RETROCOMMISSIONING AIR HANDLING SYSTEMS In The College of Applied Science and Technology (CAST), Building 70 Critical Design Review Presentation May 13th.
Plan for Today (AP Physics 2) Demonstrations, questions, and lecture on fluids.
10.3 Properties of Fluids  A fluid is defined as any matter that flows when force is applied.  Liquids like water or silver are kinds of fluid.
July 5, 2007 C. HAUVILLER CLIC stabilization Beam line and final focus.
Just add them up! 200 kPa500 kPa400 kPa1100 kPa ++=
Fluid-substrate interactions; structure of fluids inside pores.
Chapter 17.3 How do buoyancy and Archimedes’ principle relate to fluids?
Properties of Fluids 16-2.
MAJOR FINDINGS MAJOR FINDINGS  For the same reactor size, bubble size and volumetric flow rate, the bubble column had the lowest vessel dispersion number.
11/03/2014PHY 711 Fall Lecture 291 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 29: Chap. 9 of.
Partial Pressure Problems. Vocabulary Used in Partial Pressure Problems 1. Partial Pressure- The pressure of each gas in a mixture. 2. Dalton’s Law- The.
Gases Online Lecture Part 2. Gas Density and Molar Mass Using the ideal gas law and the density of a gas you can solve for the molar mass of the gas.
 Forces of attraction between particles are strong when they are close together  Particles cannot flow in a solid b/c.
VIRTUAL TEMPERATURE T V (Virtual Temp.) is the temperature a dry air parcel would be if its pressure and density were equal to a given moist air sample.
Jeopardy Q $100 Q $200 Q $300 Q $400 Q $500 Q $100 Q $200 Q $300 Q $400 Q $500 Final Jeopardy.
Chapter 1.2 Notes Pressure. All matter is made up of atoms and molecules. All matter is made up of atoms and molecules. Matter can exist in four states:
Betz revisited Prof. Guy Houlsby Department of Engineering Science Oxford Tidal Energy Workshop sponsored by the Oxford Martin School 30 th March 2012.
Baptism: No Water Down July 12, 2015 Baptism: No Water Down July 12, 2015.
10//3015PHY 711 Fall Lecture 261 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 26: Chap. 9 of.
Volume Measurement experimentally measured by liquid/gas displacement امین اله معصومی.
Chapter 15 Thermodynamics Thermodynamic Systems and Their Surroundings Thermodynamics is the branch of physics that is built upon the fundamental.
Flow of Compressible Fluids. Definition A compressible flow is a flow in which the fluid density ρ varies significantly within the flowfield. Therefore,
2.1 Fluid Flow Upthrust and flotation. Starter: test your knowledge Basic: find the density in kg m -3 Medium: state the percentage uncertainty in each.
Lecture Outline Chapter 12 College Physics, 7 th Edition Wilson / Buffa / Lou © 2010 Pearson Education, Inc.
Dr. Owen Clarkin School of Mechanical & Manufacturing Engineering Summary of Energy Topics Chapter 1: Thermodynamics / Energy Introduction Chapter 2: Systems.
Entropy Changes in Chemical Reactions.  Because entropy is a state function, the property is what it is regardless of pathway, the entropy change for.
110 th November 2010EN/CV/DC Detector Cooling Project - advancement status of Work Package N3 Thermosiphon project Michele Battistin 18 May 2011.
The reading is 7.38 mm. The reading is 7.72 mm.
Date of download: 7/8/2016 Copyright © ASME. All rights reserved. From: An Approximate Formula to Calculate the Restoring and Damping Forces of an Air.
CNT as Thermal Resistive Sensor Yu ZHANG Directed by Prof. Wen J. LI April 30, 2010.
Design of the thermosiphon Test Facilities 2nd Thermosiphon Workshop
Radiation: Particles, Waves, Rays
Gestão de Sistemas Energéticos 2016/2017
Meniscus Can estimate to the Tenths place.
waves Mechanical If a medium is needed for the transfer of energy
Asst. Prof. Dr. Hayder Mohammad Jaffal
Fig. 2 Fluidic and electrical characteristics of the wireless optofluidic system. Fluidic and electrical characteristics of the wireless optofluidic system.
Presentation transcript:

Progress Report Yu ZHANG Directed by Prof. Wen J. LI July 2, 2010

Liquid Proof-mass Accelerometer

Equilibrium Analysis Suppose at equilibrium state: From the classical ideal gas law:

Fluid in sealed channel Spring-mass system Comparisons with Spring-Mass System 4 th order 2 nd order conditionally 2 nd order

Feasibility Significant response High flow rate Big m Small k Large size Presumption: Overall size: 10mm by 10mm by 2mm Damping medium: air Moving liquid: DI water Future work to prove feasibility: Calculate the maximum liquid displacement may achieve Estimate the maximum flow rate, and compare to previous values in the CNT flow sensor project

Proposed Layouts

Feedback: Privacy Policy Feedback
Do Not Sell My Personal Information
About project: SlidePlayer Terms of Service

© 2025 SlidePlayer.com. Inc. All rights reserved.