1. A particle of positive charge q and mass m enters with velocity vj at the...
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1. A particle of positive charge q and mass m enters with velocity vj at the origin in a magnetic field B(-k) which is present in the whole space. The charge makes a perfectly inelastic collision with identical particle at rest but free to move at its maximum y-coordinate. After collision the combined charge will move on trajectory: mv where r = 9B mv A) y = qB B) (x+r)*+{y-5) - 4 C) (x-r) +(y-r) =r D) (x-r)' +| y+ 4 2. In region x>0, a uniform and constant magnetic field Bi = 2B,k exists. Another uniform and constant magnetic field B2 = B,k exists in region x<0. A positively %3D charged particle of mass m and charge q is crossing origin at time t = 0 with a velocity u = u,i. The particle comes back to its initial position after a time : (B,, u, are positive constants) 3 Tim A) 2 qB, 2 Tm В) qB, 3 πη qB, D) Particle does not come back to its initial position 1. A particle of positive charge q and mass m enters with velocity vj at the origin in a magnetic field B(-k) which is present in the whole space. The charge makes a perfectly inelastic collision with identical particle at rest but free to move at its maximum y-coordinate. After collision the combined charge will move on trajectory: mv where r = 9B mv A) y = qB B) (x+r)*+{y-5) - 4 C) (x-r) +(y-r) =r D) (x-r)' +| y+ 4 2. In region x>0, a uniform and constant magnetic field Bi = 2B,k exists. Another uniform and constant magnetic field B2 = B,k exists in region x<0. A positively %3D charged particle of mass m and charge q is crossing origin at time t = 0 with a velocity u = u,i. The particle comes back to its initial position after a time : (B,, u, are positive constants) 3 Tim A) 2 qB, 2 Tm В) qB, 3 πη qB, D) Particle does not come back to its initial position
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Principles of Taxation for Business and Investment Planning 2016 Edition
ISBN: 9781259549250
19th edition
Authors: Sally Jones, Shelley Rhoades Catanach
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