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≈ 1 m 2 c 4 /(2E 2) Details of the calculation For the photons, the travel time is T photon = d/c T neutrino = d/v ≈ (d/c)(1 m 2 c 4 /(2E 2)) T neutrino T photon = T photon m 2 c 4 /(2E 2))The maximum signal voltage is V c V m = V c (1 m) so that the maximum instantaneous output power is V c 2 R (1 m)2 = P c (1 m) 2 If the modulation index is 10 the maximum output power will be 4 P c The transmitter must be designed to carry this level of output power Types of Amplitude Modulation AM is itself divided into differentOrbital period T = 2πr/v c = (3π/Gρ)1/2 Now release a point mass from rest at r

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The momentum of the final particle is p f c = 2 pc cos(60 o) = √8 mc 2 (momentum conservation) The energy of the final particle is E F = dp/dt, E = (m 2 c 4 p 2 c 2)
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P rms c = 8538 eV λ = h/p = hc/pc = (1240 eV nm)/(8538 eV) = 0145 nm Such neutrons can be diffracted by crystals as their deBroglie wavelength is comparable with theReasoning We are asked to solve the equation of motion for a relativistic particle We have motion in two dimensions Details of the calculation (a) dp

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Aout=V c V mcos(w ct) cos(w ct) • Vm(t) is isolated using T1 – The value of Vm(t) results in Q1 to go into cutoff or saturation modes • C2 is used for couplingReasoning The equation of motion quickly yields v(t) We integrate to find x(t) Details of the calculation (a) Equation of motion F = dp/dt p = Ft E = (m 2 c 4 (Ft) 2 c 2)
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The decay of a particle is a relativistic problem In relativistic collisions energy and momentum are always conserved Details of the calculation (a) Momentum conservation requires that p = p ' (b) Energy conservation Mc 2 = 4mc 2 = (m 2 c 4 p 2 c 2)
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