Component of velocity parallel to →B i.e., vx will remain unchanged vy^j and Bj will rotate the particle in y-z plane (⊥ to →B).
At the beginning direction to magnetic force is −^k [from the relation, →F=q(vy^j×B^i)]
In the time t, particle rotates and angle θ=ωt=(Bqm)t from its original path.
In the figure we can set that, y-component of velocity at time t is vycosθ and z-component is −vysinθ.