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Can someone check my answer/solutions please
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@douglaswinslowcooper
Your solution to part A looks fine to me (I didn't check the actual numbers, but the approach looks good).
Yes. Approach to A seems correct. B. Time in region E: we know the velocity but not the length of region E, so we have to solve this from the deflection distance. use 1 cm = (1/2) (F/m) t^2, with F = qE and m the mass of the electron. this gives you the time in the E field. a = F/m. get F = qE from a = F/m C. Outside the field, no curvature (negligible gravity), just the vector sum of the final vertical and horizontal velocities calculated above (from A and from B. v=at)
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