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Vacuum books

P. Holloway, Vacuum Book Bibliography, American Vacuum Society, New York, 1982. [Pg.379]

The Manipulation of Air-Sensitive Compounds, 2nd ed., D.F. Shriver and M.A. Drezdzon, John Wiley Sons, Wiley-Interscience, New York, 1986. Not purely a vacuum book, but working in an oxygen-free environment is one of the objectives for using a vacuum. This book is the leading book in its field. [Pg.515]

Note that these equations do not contain the constants that are typically included in introductory texts, such as the vacuum permitivity constant. Theoreticians, and thus software developers, work with a system of units called atomic units. Within this unit system, many of the fundamental constants are defined as having a value of 1. Atomic units will be used throughout this book unless otherwise specified. [Pg.8]

The other vacuum option is a simple little aspirator that attaches to ones faucet or hose. This 15 device pulls a decent vacuum however, it is not an option at all in Strike s book. Running one of these babies 10-12 hrs a day is a despicable waste of a community s water supply. [Pg.16]

The solvent is then washed 3 x 50mL dH20 and, if desired, can be washed once with lOOmL saturated NaCI solution. Finally, the solvent is dried through Na2S04, removed by vacuum distillation, and the first 5 to 10mL of oil that distills over is saved because it is isomerized safrole (iososafrole), which is suitable for reuse. The rest of the oil that comes over will be the ever lovely MD-P2P, which is perfectly suitable for amination by any method given in this book. [Pg.89]

Ether - Starting fluid (works great - Quaaaaack ) 2. Home made mercuric acetate (Now this stuff can be special ordered from ones chem supplier but there s a delay, may look funny - Quaaaaack , and is more expensive. So what is the solution to this Make it yourself Its easy, quantitative, and cheaper. Strike mentions this in the book and points ducks to a reference. Follow the EXACT same procedure for Mercuric Propionate except use glacial acetic acid...quack ). You ll need to use 20 to 25% more of the home brew mercuric acetate since it is a little contaminated with acetic (ducks can t get it totally dry without a vacuum oven). 3. NaOH washed Brazillian is fine Quack No need to purify further for starting material ... [Pg.90]

Vacuum filtering can be a bit tricky, as the filter paper clogs up very quickly and stalls the process. With this stuff it is particularly important to get rid of as much of the solids as possible or your distillation be will very messy. A way round that I have found (that isn t in any book) was to use loads of filter papers, throw them all into a big beaker and then rinse them with solvent, then filter the solvent. Filter tiny amounts at a time, as soon as the paper blocks - stop and change the paper. I normally run the filtrate through at least twice. Any way you can make sure that you have done two... [Pg.226]

The present book brings to the reader a state-of-the-art treatment of high-pressure shock compression of solids in a type of tutorial manner. It has been felt by the shock physics and engineering communities that there is a need for such a book to aid the education and training of undergraduate and graduate students of physics and engineering. We hope that the present book will partially fill that vacuum. We certainly welcome any comment or criticism on the content of this book, in the hope that these will be incorporated into later editions of the book. [Pg.401]

Historically, EELS is one of the oldest spectroscopic techniques based ancillary to the transmission electron microscope. In the early 1940s the principle of atomic level excitation for light element detection capability was demonstrated by using EELS to measure C, N, and O. Unfortunately, at that time the instruments were limited by detection capabilities (film) and extremely poor vacuum levels, which caused severe contamination of the specimens. Twenty-five years later the experimental technique was revived with the advent of modern instrumentation. The basis for quantification and its development as an analytical tool followed in the mid 1970s. Recent reviews can be found in the works by Joy, Maher and Silcox " Colliex and the excellent books by Raether and Egerton. ... [Pg.137]

Hollomon s ethos, combined with his ferocious energy and determination, and his sustained determination to recruit only the best researchers to join his group, over the next 15 years led to a sequence of remarkable innovations related to materials, including man-made diamond, high-quality thermal insulation, a vacuum circuit-breaker, products based on etched particle tracks in irradiated solids, polycarbonate plastic and, particularly, the Lucalox alumina envelope for a metal-vapour lamp. (Of course many managers besides Hollomon were involved.) A brilliant, detailed account of these innovations and the arrangements that made them possible was later written by Guy Suits and his successor as director, Arthur Bueche (Suits and Bueche 1967). Some of these specific episodes will feature later in this book, but it helps to reinforce the points made here about Hollomon s coneeption of broad research on materials if I point out that the invention of translucent alumina tubes for lamps was... [Pg.9]

My principal objective in Section 10.4 has been to underline the necessity for a drastic enhancement of a crucial experimental technology, the production of ultrahigh vacuum, as a precondition for the emergence of a new branch of science, and this enhancement was surveyed in the preceding Section. It would not be appropriate in this book to present a detailed account of surface science as it has developed, so 1 shall restrict myself to a few comments. The field has been neatly subdivided among chemists, physicists and materials scientists it is an ideal specimen of the kind of study which has flourished under the conditions of the interdisciplinary materials laboratories described in Chapter 1. [Pg.407]

By permission, Ryans, J. L. and Roper, D. L., Process Vacuum System Design and Operation, McGraw-Hill Book Co. Inc., 1986 [18J. [Pg.133]

Figure 2-46. Typical flow velocities for vacuum lines. Note 1 torr = 1.33 mb = 133.3 Pa. 1.0 ft/sec = 0.3048 m/seo. By permission, Ryans, J. L. and Roper, D. L., Process Vacuum System Design Operation, McGraw-Hill Book Co., Inc., 1986 [18]. Figure 2-46. Typical flow velocities for vacuum lines. Note 1 torr = 1.33 mb = 133.3 Pa. 1.0 ft/sec = 0.3048 m/seo. By permission, Ryans, J. L. and Roper, D. L., Process Vacuum System Design Operation, McGraw-Hill Book Co., Inc., 1986 [18].
LaPelle, R. R., Practical Vacuum Systems, 1972, McGraw-Hill Book Co., 1st Ed. [Pg.398]

The heaviest bottoms product from the main column is commonly called slurry or decant oil. (In this book, these terms are used interchangeably.) The decant oil is often used as a cutter stock with vacuum bottoms to make No. 6 fuel oil. High-quality decant oil (low sulfur, low metals, low ash) can be used for carbon black feedstocks. [Pg.23]

On the other hand, all the solvents with which we deal in this book have large electrostatic susceptibilities. In Fig. 4b the length of the vertical arrow C is almost as great as B. That is to say, the amount of free energy lost by the dielectric is almost as large as the whole of the energy initially associated with the field X in the vacuum. [Pg.11]

The Amount of Free Energy Lost by a Dielectric. The above considerations apply to fields of any intensity. When we are dealing only with ordinary weak fields, for which the polarization is proportional to the field (the straight part of the curve in Fig. 5), the substance under discussion is said to possess a dielectric constant. This will be denoted by t. In a vacuum e is set equal to unity and in a dielectric the polarization is proportional to (t — 1). The loss of free energy by the dielectric may be expressed in terms of e. In Note 1 of the Appendix at the end of this book it is shown that, when a homogeneous slab is introduced into a uniform field of initial intensity X, the free energy lost per unit volume amounts to... [Pg.13]

It is important to understand that this material will not be presented in a theoretical vacuum. Instead, it will be presented in a particular context, consistent with the majority of the author s experience, namely the development of calibrations in an industrial setting. We will focus on working with the types of data, noise, nonlinearities, and other sources of error, as well as the requirements for accuracy, reliability, and robustness typically encountered in industrial analytical laboratories and process analyzers. Since some of the advantages, tradeoffs, and limitations of these methods can be data and/or application dependent, the guidance In this book may sometimes differ from the guidance offered in the general literature. [Pg.2]

All equations given in this text appear in a very compact form, without any fundamental physical constants. We achieve this by employing the so-called system of atomic units, which is particularly adapted for working with atoms and molecules. In this system, physical quantities are expressed as multiples of fundamental constants and, if necessary, as combinations of such constants. The mass of an electron, me, the modulus of its charge, lei, Planck s constant h divided by lit, h, and 4jt 0, the permittivity of the vacuum, are all set to unity. Mass, charge, action etc. are then expressed as multiples of these constants, which can therefore be dropped from all equations. The definitions of atomic units used in this book and their relations to the corresponding SI units are summarized in Table 1-1. [Pg.21]

The lowest level of the conduction band for metals Vc and the highest level of the valence band for semiconductors is very often used as a reference point for the energies of the Fermi levels in this book, however, the energy of a free electron at rest in a vacuum will be used as the reference point for the scale of the Fermi levels (cf. Fig. 3.2.). [Pg.159]

Holland, L., Vacuum Deposition of Thin Films. Chapman Hall, London, 1960. 4B. Smithells, C. J., (Ed.) Metals Reference Book, 4th Ed., Vol. 1. Butterworth, London, 1967. [Pg.186]

The content of the book is based on the 6-h-per-week lecture course which one of us (G. Ventura) has given at the University of Florence between 2001 and 2006. In authors intents, the book should stand alone as a practical guide to cryogenics. For this reason, a brief chapter about vacuum techniques precedes the cryogenic items. [Pg.14]


See other pages where Vacuum books is mentioned: [Pg.24]    [Pg.57]    [Pg.69]    [Pg.1326]    [Pg.256]    [Pg.358]    [Pg.365]    [Pg.123]    [Pg.261]    [Pg.2]    [Pg.4]    [Pg.7]    [Pg.530]    [Pg.24]    [Pg.30]    [Pg.203]    [Pg.205]    [Pg.189]    [Pg.335]    [Pg.854]    [Pg.14]   
See also in sourсe #XX -- [ Pg.98 ]




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