Animated Solution for Physics - Magnetic Effects of Current: A beam of protons with a velocity 4×105 m/s enters a uniform magnetic field of 0.3 T at an angle of 60∘ to the magnetic field. Find the radius of the helical path taken by the protons beam. Also find the pitch of the helix (which is the distance travelled by a proton in the beam parallel to the magnetic field during one period of rotation).
Visualized Solution
Visualizing the Helical Path
The proton enters the magnetic field B at an angle θ=60∘.
The velocity v can be resolved into two components:
1. Parallel to B: v∥=vcosθ
2. Perpendicular to B: v⊥=vsinθ
The Physics of the Helix
The perpendicular component v⊥ provides the centripetal force, causing circular motion.
The parallel component v∥ is unaffected by the magnetic field, causing linear motion.
The superposition of these two motions results in a helical path.
r=qBmv⊥
The radius r of the circular cross-section depends only on the perpendicular velocity.
r=qBmvsinθ
Substituting Values for r
Given:
m=1.67×10−27 kg
v=4×105 m/s
θ=60∘
B=0.3 T
q=1.6×10−19 C
r=(1.6×10−19)(0.3)(1.67×10−27)(4×105)(sin60∘)
Calculating the Radius
sin60∘=23≈0.866
r=1.6×0.31.67×4×0.866×10−27+5+19
r=0.485.785×10−3
r=12.05×10−3 m
r≈1.2×10−2 m
p=v∥T
The pitch p is the linear distance traveled along the magnetic field during one complete rotation.
The Sigma Insight: Motion of a Charge in Magnetic Fields
Solution Diagram
The Anatomy of a Helix
Imagine you are a proton, fired out of a particle accelerator at a blistering speed of 4×105 m/s. Suddenly, you enter a region permeated by a uniform magnetic field of 0.3 T. If you had entered perfectly perpendicular to the field, you would be trapped in an endless, flat circular orbit. If you had entered perfectly parallel, you would feel absolutely no force and continue in a straight line forever.
But in this scenario, you enter at a rebellious angle of 60∘. What happens now?
To understand the physics, we must invoke the principle of superposition. We break your velocity vector v into two independent components:
1. The Perpendicular Component (v⊥): This component is perpendicular to the magnetic field. According to the Lorentz force law, F=q(v×B), this component generates a constant force that acts as a centripetal force, whipping you into a circular frenzy.
2. The Parallel Component (v∥): This component is perfectly aligned with the magnetic field. Because the cross product of parallel vectors is zero, the magnetic field exerts absolutely zero force on this component. It acts like a ghost, carrying you forward at a constant speed.
When you combine a circular motion with a constant forward translation, you trace out a beautiful, three-dimensional helix.
Decoding the Circular Dance
Finding the Radius
Let's calculate the radius of the circular part of your helical journey. The magnetic force provides the centripetal force:
qv⊥B=rmv⊥2
Solving for the radius r, we get:
r=qBmv⊥=qBmvsinθ
Now, we simply substitute the standard constants for a proton (m=1.67×10−27 kg, q=1.6×10−19 C) and our given values:
r=(1.6×10−19)(0.3)(1.67×10−27)(4×105)(sin60∘)
Knowing that sin60∘=23≈0.866, the arithmetic simplifies beautifully:
r=0.481.67×4×0.866×10−3≈1.2×10−2 m
The Forward March
Calculating the Pitch
The pitch of a helix is the linear distance you travel forward along the magnetic field during exactly one complete circular rotation. Think of it as the distance between two adjacent threads on a screw.
To find the pitch, we need to know how long one rotation takes. This is the time periodT. The beauty of cyclotron motion is that the time period is completely independent of your velocity!
T=v⊥2πr=v⊥2π(qBmv⊥)=qB2πm
During this time T, your parallel velocity v∥ has been carrying you forward. Therefore, the pitch p is:
p=v∥×T=(vcosθ)(qB2πm)
Let's plug in the numbers, noting that cos60∘=0.5:
p=(1.6×10−19)(0.3)(2π)(1.67×10−27)(4×105)(0.5)
p=0.486.28×1.67×2×10−3≈4.37×10−2 m
The Grand Finale
By simply decomposing a vector, we've completely mapped out a complex three-dimensional trajectory. The proton spirals through the magnetic field with a radius of 1.2 cm, advancing forward by 4.37 cm with every single loop. This exact principle is what governs the spectacular auroras at the Earth's poles, where charged particles from the solar wind spiral along the Earth's magnetic field lines!