`m = 1.6xx10^(-27) kg, q = 1.6xx10^(-19)C`
`B = 1 T`
` v = 10^(7) m//s`
`F = q .v B sin alpha`
(acting towards ` O` by Fleming's left hand rule )
rArr ` F = qvB` `[:. alpha = 90^(@)]`
But ` F = ma`
:. ` qvB = ma :. a = (qvB)/(m)`
` = (1.6xx10^(-19)xx10^(7)xx1)/(1.6xx10^(-27)`
` = 10^(15) m//s^(2)`
`/_OEF = 45^(@)` ` (because OE act as a radius)`
By symmetry `/_OFE = 45^(@)`
:. `/_EOF = 90^(@)` ( by Geometry)
This is the centripetal acceleration
:. `(v^(2))/(r) = 10^(15) rArr r = (10^(14))/(10^(15)) = 0.1 m`.
Therefore ` EF = 0.141 m`.
If the magnetic field is in the outward direction and the particle enters in the same way at `E` , then according to Fleming's left hand rule, the particle will turn towards clockwise direction and cover `3//4th` of a circle as shown in the figure.
Time required `= (3)/(4)xx [(2 pir)/(v)] = 4.71xx10^(-8) sec`.
