Electric field and magnetic fiedl `n` a region of sace is given by `E=E_0hatj` and `B=B_0hatj`. A particle of specific charge alpha is released from origin with velocity `v=v_0hati`. Then path of particel

Electric field and magnetic field n a region of space is given by E=E_0hatj and B=B_0hatj . A particle of specific charge alpha is released from origin with velocity v=v_0hati . Then path of particle

Electric field and magnetic field in a region of space are given by (Ē= E_0 hat j) . and (barB = B_0 hat j) . A charge particle is released at origin with velocity (bar v = v_0 hat k) then path of particle is

Electric field and magnetic field in a region of space are given by (Ē= E_0 hat j) . and (barB = B_0 hat j) . A charge particle is released at origin with velocity (bar v = v_0 hat k) then path of particle is

In a certain region, uniform electric field E=-E_0hatk and magnetic field B = B_0hatk are present. At time t = 0 , a particle of mass in and charge q is given a velocity v = v-0hatj + v-0hatk . Find the minimum speed of the particle and the time when it happens so.

A proton is fired from origin with velocity vecv=v_0hatj+v_0hatk in a uniform magnetic field vecB=B_0hatj .

The electric field acts positive x -axis. A charged particle of charge q and mass m is released from origin and moves with velocity vec(v)=v_(0)hatj under the action of electric field and magnetic field, vec(B)=B_(0)hati . The velocity of particle becomes 2v_(0) after time (sqrt(3)mv_(0))/(sqrt(2)qE_(0)) . find the electric field:

In the region between the plane z=0 and z=a (a gt 0) , the uniform electric and magnetic fields are given by vecE=E_(0)(hatk-hatj) , vecB=B_(0)hati . The region defined by a le z le b contains only magnetic field vecB= -B_(0)hati . Beyond z gt b no field exits. A positive point charge q is projected from the origin with velocity v_(0)hatk . Assuming the mass of the particle to be (2)/(3)(qE_(0)a)/(v_(0)^(2)) . The value of E_(0) such that the particle moves undeviated upto the plane z=a is

Electric field strength vecE = E_0 hati and vecB = B_0 hati exists in a region. A charge is projected with a velocity vecv = v_0 hatj origin, then