When a charged particle is projected at an angle θ to a magnetic field, the component of velocity parallel to the field is vcosθ while perpendicular to the field is vsinθ, so the particle will move in a circle of radius
r=m(vsinθ)qB=(1.67×10−27)×(4×105×sin600)1.6×10−19×0.3=(1.67×10−27)×(4×105×√32)1.6×10−19×0.3=2×10−2√3
Time period: T=2πrvsinθ=2π×2×10−2√34×105×sin600=2π×2×10−2√34×105×√32=2π3×10−7
Pitch: P=vcosθT=(4×105)×cos600×2π3×10−7=4π3×10−2=4.35×10−2m