Appendix: Problem Index 627
9.2.9 Emulsions
Range-energy graph for^2 H and^3 He 9.66
9.2.10 Motion of Charged Particles in Magnetic Field
p= 0 .3Br 9.67
An energetic proton heading toward earth’s centre just
misses it9.68
Null deflection in crossedEandB 9.69
Mass of particle fromEandr 9.70
Deflection of a particle in magnetic field 9.71
An electron recrossingx-axis in electric field 9.72
Radius of curvature of helical path 9.73
A proton circling around magnetic equator 9.74
Power delivered to earth by cosmic rays 9.75
Mass spectroscopy of kaons 9.76
9.2.11 Betatron
Electron energy 9.77
Number of revolutions,Emaxand<E> 9.78
9.2.12 Cyclotron
KE in terms ofrandB 9.79
Field strength and acceleration time 9.80
ΔBfor cyclotron resonance 9.81
Resonance condition forP,D,α 9.82
Range of frequency modulation in synchrocyclotron 9.83
Calculation ofBandrfor givenEmaxandf 9.84
Drop ofBfor cyclotron resonance when alphas are accelerated
instead of deuterons9.85
Tmaximparted to electron from proton collision 9.86
To calculate final frequency from given initial frequency andEmax
for protons9.87
9.2.13 Synchrotron
Rof protons for givenBandE 9.88, 89
Percentage depth of modulation 9.90
Energy loss in electron synchrotron 9.91
Derivation ofR=m 0 c(n^2 + 2 n)^1 /^2 /qB,n=T/m 0 c^2 9.92
Proton energy when B rises to known value 9.93
Acceleration of D and^3 He when protons are replaced 9.94
GivenB,V,φsandTmaxfor protons, to findr,tto calculateΔf
(initial), frequency modulation range9.95
Feasibility of 500 GeV electron synchrotron 9.96
KE of proton in known orbit making 1 revolution/μs9.97
For an electron synchrotron to find initial RF, total time and
distance traveled