In an electron-diffraction arrangement using a nickel crystal (d=0.091nm), the second-order intensity maximum is observed at a glancing angle of 65∘.
a. (i) Calculate the potential difference V1 through which the electrons were accelerated. Take h=6.626×10−34Js, me=9.11×10−31kg and e=1.6×10−19C.
b. (ii) If the accelerating potential is increased by 200V while keeping all other conditions unchanged, determine the new glancing angle θ2 at which the first-order maximum will now appear.
c. (iii) Briefly justify whether the angular separation between successive maxima will increase or decrease as the accelerating potential is raised, keeping the crystal the same.