## Journal of the Franklin Institute, Volume 266Pergamon Press, 1958 Vols. 1-69 include more or less complete patent reports of the U. S. Patent Office for years 1825-1859. cf. Index to v. 1-120 of the Journal, p. [415] |

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**constant**, ŋ = a**constant**are solutions of Eqs . 1 . The second class of solutions is sometimes called simple waves . The theory of simple waves is amply discussed in ( 2 ) . Let us recall that a simple wave is defined as a region in ...Page 161

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**constant**thrust and**constant**gravitation . The central result for this problem is that p ( t ) is**constant**, given by tan = & b / √no2 + 2gnь . ( 3.1 ) This result holds for any form of the function T ( t ) . The values of έ , ь , and ...Page 460

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**constant**velocity relative to the laboratory . On the other hand the laboratory frame inertial force does not vanish under condi- tions of**constant**velocity . This is because the rest mass of the grain changes as it is polarized or ...### Contents

JULY 1958 No | 1 |

Effects of Unipolar Air Ions on Microorganisms and on Evaporation | 9 |

Plastics in the Space Age JOHN H Lux | 21 |

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acceleration accelerometer analysis angle applied Atomic attacking moments axis Bell Telephone Laboratories Benjamin Franklin Parkway Chairman chapter coefficients Committee components conjugate frames constant diagrams difference equations discussion Donald Wills Douglas Earth effect electrical electronic energy Engineering error ferrocene field flight fluid force Franklin Institute Franklin Institute Laboratories function gyro gyroscope heat hinge rotations inertial guidance inertial guidance system initial instrument LEPAGE linear load M₁ mass material mathematical mechanism Medal method momentum navigation nuclear obtained operation paper particles perturbation Phila Philadelphia physical plastic platform position Poynting theorem present Price problem proper frame radius range reactor reference rest mass rocket Science shown in Fig solution space techniques temperature theory tion torque trajectory transformation tube velocity voltage York z-transform zero Δφ