Magnetron Diode Oscillations

Osepchuk, John M.

doi:10.1016/b978-0-12-395553-1.50028-5

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1964

2018

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Cited by 8 publications

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“…Forming the square of Eqs. 5*13 and 5.1^ and differentiating with respect to time gives ft [(P y ) 2 + (P z -qB y)2 J +^( 2q r. rp) = o ,(5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15) which implies ^ [Py + (P z -q B y) 2 ] + q (J>(y,z) = C , (p.lb)where C ■ constant.iThe left-hand side of this last equation is simply H as given by Eq. 5«10« Thus for a conservative system H (y, z, p .…”

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confidence: 99%

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Analysis of Crossed-Field Space-Charge Flows

Masnari¹

1964

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“…5«10« Thus for a conservative system H (y, z, p . P_, t) = constant(5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17) along any given trajectory. In this case it is also true that H is equal to the total energy of the electron at any point.…”

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confidence: 99%