Fun games with membranes and cold traps. I will assume: The total volume is 4000 l. The circulation speed X l/h = Y l/h = 200 l/h pump speed. The volume.

Slides:



Advertisements
Similar presentations
CHEMICAL AND PHASE EQUILIBRIUM (1)
Advertisements

Chemistry An Introduction to General, Organic, and Biological Chemistry, Eleventh Edition Copyright © 2012 by Pearson Education, Inc. Chapter 6 Gases 6.8.
A User-Friendly, Two-Zone Heat Release and Emissions Model Jeremy Cuddihy Major Professor: Dr. Steve Beyerlein.
Physical Chemistry I (TKK-2246)
1 Chapter 6 Gases 6.8 Partial Pressures (Dalton’s Law) Copyright © 2009 by Pearson Education, Inc.
© 2013 Pearson Education, Inc. Chapter 7, Section 9 General, Organic, and Biological Chemistry Fourth Edition Karen Timberlake 7.9 Partial Pressures (Dalton’s.
Physical Characteristics of Gases
Thermodynamics & Gas dynamics of Real Combustion in Turbo Combustor P M V Subbarao Professor Mechanical Engineering Department Tools for precise estimation.
Chapter 4 Mass and Energy Analysis of Control Volumes (Open Systems)
Chapter 9 Combining Reactions and Mole Calculations.
Chapter 9 Combining Reactions and Mole Calculations.
WHAT DO THE COEFFICIENTS IN A REACTION TELL US??!?!
Department of Mechanical Engineering ME 322 – Mechanical Engineering Thermodynamics Lecture 28 Internal Combustion Engine Models The Otto Cycle The Diesel.
Kinetics Class #4 OB: reactions that are in dynamic equilibrium and how to “push” them forward, or reverse using LeChatelier's Principle.
Chapter 16 Chemical and Phase Equilibrium Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 5th edition by Yunus.
Chapter 16: Chemical Equilibrium- General Concepts WHAT IS EQUILIBRIUM?
Lec.11 Liquid State & Solution. Solution may be defined as a homogeneous mixture of two or more substances whose composition can be continuously varied.
AE 412 THERMODYNAMIC CYCLE SIMULATION II Prof.Dr. Demir Bayka.
Temperature and Pressure
The particle nature of matter: revision. You should be familiar with the characteristic properties of solids, liquids and gases from your junior science.
1) Take out your homework 2) What is solubility and how can it be changed.
Chapter 14 Chemical reactions
1 Chapter 6 The States of Matter 6.9 Partial Pressure (Dalton’s Law)
1 Section II Respiratory Gases Exchange 2 3 I Physical Principles of Gas Exchange.
Thermodynamic Cycles Air-standard analysis is a simplification of the real cycle that includes the following assumptions: 1) Working fluid consists of.
Department of Mechanical Engineering ME 322 – Mechanical Engineering Thermodynamics Lecture 31 Ideal Gas Mixtures.
Chemical Quantities Standards 3b. Students know the quantity of one mole is set by defining one mole of carbon-12 atoms to have a mass of exactly 12.
Dalton’s Law Mixtures of Gases. Introduction From the kinetic theory of gases, at a given temperature and in a given volume gas pressure depends only.
Quantitative Chemistry
Engineering Chemistry 14/15 Fall semester Instructor: Rama Oktavian Office Hr.: M.13-15, Tu , W , Th ,
1 Lecture 6 Gases Properties of Gases Gas Pressure Copyright © 2007 by Pearson Education, Inc. Publishing as Benjamin Cummings.
 The average kinetic energy (energy of motion ) is directly proportional to absolute temperature (Kelvin temperature) of a gas  Example  Average energy.
SOLUBILITY BY DR ABDUL JALIL ASSISTANT PROFESSOR DEPARTMENT OF ANAESTHESIA AND ICU LAHORE GENERAL HOSPITAL/PGMI LAHORE.
1 Physical Characteristics of Gases Chapter Kinetic-molecular theory Particles of matter are always in motion.
Molar Volume. Avagadro’s Principle Equal volumes of gases contain equal numbers of molecules Volume of a gas varies directly with the number of molecules.
Advance Chemical Engineering Thermodynamics
Homework Check (The Ideal Gas Law) 1.If I contain 3 moles of gas in a container with a volume of 60 L at a temperature of 400 K, what is the pressure inside.
PREMIERE QUESTION. c) Determine the final pressure in the vessel in mbars d) Assuming that CO 2 behaves nonideally, determine its partial pressure at.
Gases. I.Real Gases (we will not study these much) A. Do NOT apply the Kinetic Molecular Theory 1. The particles in a real gas can NOT be thought of as.
1 KHS ChemistryUnit 2.2 Equilibrium Chemistry Equilibrium Chemistry Adv Higher Unit 2 Topic 2 part 1 Gordon Watson Chemistry Department, Kelso High School.
Gases Ch.10 and 11. Kinetic-Molecular Theory 1.Gases consist of very small particles that are far apart Most particles are molecules Volume of particles.
Chapters 10 and 11: Gases Chemistry Mrs. Herrmann.
Active gas system status. S.Konovalov, K.Zhukov. Active gas system operation. S.Konovalov "Active gas system..."TRT Overview  Good design.
Section Six.
The Simplest Phase Equilibrium Examples and Some Simple Estimating Rules Chapter 3.
GASES.
Chapter 14 Chemical Equilibruim. Objectives Describe chemical equilibrium Write an equilibrium constant expression Calculate the equilibrium constant.
General, Organic, and Biological Chemistry Copyright © 2010 Pearson Education, Inc. 1 Chapter 7 Gases 7.9 Partial Pressure (Dalton’s Law)
حرارة وديناميكا حرارية
KINETIC MOLECULAR THEORY Physical Properties of Gases: Gases have mass Gases are easily compressed Gases completely fill their containers (expandability)
The Ideal Gas Law No gas perfectly obeys all of the gas laws under all conditions. Nevertheless, these assumptions work well for most gases and most conditions.
Kinetic-Molecular Theory and Gas Laws Kinetic-Molecular Theory and Gas Laws.
Solution Equilibrium and Factors Affecting Solubility
 Solid: maintains a fixed volume and shape  Liquid: maintains a fixed volume but takes the shape of the container  Gas: occupies the entire volume.
1910 Nobel Prize van der Waals On the continuity of the gaseous and liquid state (1872) … if a gas in the extremely dilute state, where the volume is.
GASES. Gases  The physical state of gases is defined by several physical properties  Volume  Temperature  Amount (commonly expressed as number of.
Chapter Nineteen: Solutions  19.1 Water  19.2 Solutions  19.3 Acids, Bases, and pH.
CHAPTER 2 Matter and Change. What is Matter?  Matter is anything that has mass and takes up space  Mass = the amount of matter an object contains 
Avogadro's Principle “Equal volumes of gases at the same temperature and pressure contain equal numbers of particles” It doesn’t matter what type of gas.
Houston Community College System Chemistry 1405 Chapter 5 The Physical Properties of Gases By Mounia Elamrani Blei / Odian ’ s General, Organic, and Biochemistry.
1 Chapter 6 Gases 6.1 Properties of Gases 6.2 Gas Pressure Copyright © 2009 by Pearson Education, Inc.
Chapter Nineteen: Solutions  19.1 Water  19.2 Solutions  19.3 Acids, Bases, and pH.
Gas Exchange and Pulmonary Circulation. Gas Pressure Gas pressure is caused by the molecules colliding with the surface. In the lungs, the gas molecules.
Wednesday, October 7 th  Please take out your notes!  A gas mixture with a total pressure of 745 mmHg contains each of the following gases.
Solution of Thermodynamics: Theory and applications
8.8 Partial Pressure (Dalton’s Law)
Gas Stoichiometry.
1910 Nobel Prize van der Waals
Presentation transcript:

Fun games with membranes and cold traps. I will assume: The total volume is 4000 l. The circulation speed X l/h = Y l/h = 200 l/h pump speed. The volume is divided into N steps where N=V/X=20 with no diffusion between the steps. The total volume which is rejected at the exhaust is replaced by pure C 4 F 10. The total volume,  V i, which is pumped out at stage i for one step, is transferred to stage i+1 as one volume and then treated at this membrane in 100 mini steps assuming that the partial pressures do not change significantly during a mini step. (This statement is perhaps overly optimistic, but I checked that there is no real difference between 100 and 500.) 1 (I stopped at n=4)

Neomechs CO l/h/mbarp1-p26000 mbar Ar l/h/mbarp3-p41000 mbar O l/h/mbarp5-p6300 mbar N l/h/mbarp7-p8120 mbar CF l/h/mbar C 4 F l/h/mbar 5% air in the C 4 F 10 volume. Numbers from an old logbook 2

Small losses of C 4 F 10 and reasonable purity. (1 % N 2 ) but not fast. 3

Switch off Stage I and use p3-p46000mbar p5-p61000mbar p7-p8200mbar Still tolerable losses for the same purity. 4

Switch off Stage I and II and use p5-p66000mbar p7-p8500mbar Not too surprisingly, the losses are now rather high. 5

CO 2 is easy. For a 5% admixture use p1-p22000mbar p3-p41000mbar p5-p6500mbar p7-p850mbar 6

What about a steady state air leak? Try with 0.5 l/h. That is 0.5 l/h C 4 F 10 []  and 0.5 l/h air []  use p1-p26000mbar p3-p41000mbar p5-p6500mbar p7-p8120mbar and start the membranes when there is 2% air in the volume. Not perhaps the most optimal device for such a state. Still, it will stabilise around 98.5%. The rest being N 2. 7

The fiddling with the pressures is very depending on the actual (measured) throughput of the membranes. The pressures should probably also be adjusted as a function of the admixture in the gas. Look for another type in my old logbook: Generon CO l/h/mbar Ar O N CF C 4 F and use p1-p22000mbar p3-p4500mbar p5-p6100mbar p7-p820mbar Start out with 5 % air 8

9 Will now have a look at gas scrubbing at low temperature. Have used: Tables of Physical and Chemical Constants Physical Properties and gas Solubilities, Journal of Chemical and Engineering Data Vol. 18 No Solubility of gases in fluorocarbons, 3M pub M.F. Costa Gomes et al., Journal of Fluorine Chemistry 125(2004)1325 Ostwald solubility coefficient. Volume of gas dissolved in unit volume at ambient temperature and pressure. In anesthetic practice, these are quoted in tables, assuming a body temperature of 37°C. Note that the volume of gas dissolved is only dependent on temperature, and not pressure (though the number of molecules and the activity of these is pressure-dependent). This differs from Bunsen's solubility coefficient (a) in that the amount of dissolved gas is expressed in terms of its volume at the temperature of the experiment, instead of STPD. Friedrich Wilhelm Ostwald Nobel Prize in Chemistry in 1909 The mole Kingdom:Animalia Phylum:Chordata Class:Mammalia Infraclass:Eutheria Order:Soricomorpha Family:Talpidae Which has taken me through a tour of mole units and Ostwald's coefficient. Just to get (cc gas) in (cc liquid) at a given temperature and partial pressure. It does indeed require some rather large extrapolations (and faith).

10 Water is well known. Compare 3M numbers at one temperature with measurements at many different temperatures. Looks consistent.

11 Use the same set-up as for the membranes. That is Total volume: 4000 l Circulation: 200 l/h → 20 steps No diffusion and no compressibility. Total volume of the scrubber: 2 l 3 bar < scrubber pressure <3.5 bar Pressure stabilizing gas : He at 5 l/h Each step split in 500 mini steps. Checked that there is no real difference between 500 and 1000 steps (apart from time used on my PC).

12 Time (h)C 4 F 10 N 2 O 2 He Composition (%) Start with 5 % air and the cold trap at - 60 degC

13 N 2 will also work fine, but will end up with some 2.5 %. This is less than what I would have expected from some measurements at COMPASS and could indicate that the solubility constants that I am using are too low by about a factor of two. C 4 F 10 N 2 O

14 C 4 F 10 N 2 O 2 He C 4 F 10 N 2 O 2 He No real change in purity, but a rather dramatic increase in losses. CO 2 will not work in a cold trap.

15 Some sort of a Conclusion. Gas scrubbing, cold trap at (at least) -60 degC, is the best choice if the aim of the game is to get air content in the range of ppm. The triple membrane contraption will give oxygen content of about 0.1 % nitrogen of <1 % without any excessive loss of C 4 F 10 A steady state leak, would be better handled with a cold trap. The principle of Gas Scrubbing can easily be understood from one clear sketch found in freepatents.com