Aircraft Illustrated Special: RAF Phantom by Peter R. Foster

By Peter R. Foster

Humble BeginningsTactical PhantomsUK Air DefenceAir Defence RAF GermanyFalklands PhantomsIndividual airplane Histories

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3. 4. 5. 9. 10. 11. Mass Spectrometer Leak Detectors for Other Tracer Gases and Future Developments in Leak Detection References 9. 1. 1. 2. 2. 1. 2. 3. 4. 3. 1. 1. 2. 2. 1. 2. 3. 4. 4. 1. 2. 1. 2. Network Approach General References 10. GasSurface Interactions and Diffusion John B. 1. 1. 2. 3. 4. 5. 6. 7. 8. 2. 1. 2. 3. 4. 5. 6. 3. 4. 1. 2. 3. 4. 5. 6. 7. Bakeout Processes References 11. Ultrahigh and Extreme High Vacuum Paul A. 1. 1. 2. 3. 4. 2. 1. 2. 3. 3. 4. 1. 5. UHV/XHV Hardware 620 620 622 625 628 629 636 639 641 642 642 643 646 647 648 648 652 652 References 12.

1. 2. 3. 4. 5. 6. 7. 8. 2. 1. 2. 3. 4. 5. 6. 3. 4. 1. 2. 3. 4. 5. 6. 7. Bakeout Processes References 11. Ultrahigh and Extreme High Vacuum Paul A. 1. 1. 2. 3. 4. 2. 1. 2. 3. 3. 4. 1. 5. UHV/XHV Hardware 620 620 622 625 628 629 636 639 641 642 642 643 646 647 648 648 652 652 References 12. 1. 1. 2. 3. 4. 2. 3. 1. 2. 3. 4. 4. 5. Measurement of Pumping Speeds References Appendix Graphic Symbols for Vacuum Components Conversion Factors for Pressure Units Vapor Pressure of Common Gases Vapor Pressure of Solid and Liquid Elements General Reference Books on Vacuum Science and Technology 665 670 673 676 676 680 683 686 689 692 695 701 701 708 709 711 714 Index < previous page 715 page_xxi next page > < previous page page_xxiii next page > Page xxiii Acronyms Acronyms used in the text are listed under the chapter where they occur.

Note that we could have assumed the second molecule to have any value of a velocity component u2 other than zero orthogonal to < previous page page_11 next page > < previous page page_12 next page > Page 12 the line of centers, but this component would have no effect on the final velocity of the first molecule as given by Eq. 46). If we consider only orthogonal collisions in which the first molecule is repeatedly struck in successive collisions by one of the other molecules with a velocity component v2 which is a constant equal to the most probable velocity, vm, and assume that the initial u1 = vm also, then N successive orthogonal collisions would give a final speed By a process of reasoning similar to that for calculating the rate of absorbtion of a molecular beam by scattering in a gas [14], it can be shown that the probability of N + 1 or more successive orthogonal collisions, without collisions of another type, is which is the probability that the speed of m1 is equal to or greater than W1(0 < W1 < ∞), where b is a constant to be determined.

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