The Crossed-Field Setup
Imagine a charged particle entering a region where both an electric field and a magnetic field are present. This is a classic "crossed-field" setup, often used in velocity selectors and mass spectrometers. Our particle, with a specific mass and charge, enters this region at the origin, moving purely along the positive x-axis with a velocity v=1.28×106i^ m/s.
The electric field E points downwards along the negative z-axis, while the magnetic field B points along the positive y-axis. To understand the particle's journey, we must analyze the forces acting on it.
The Balancing Act
Lorentz Force
The total force on a charged particle in electromagnetic fields is given by the Lorentz force equation:
Let's break this down. First, the electric force Fe=qE. Substituting the given values, we find that the electric force pulls the particle downwards along the negative z-axis with a magnitude of 1.6384×10−14 N.
Now, what about the magnetic force? Using the right-hand rule for the cross product v×B (where v is along +x and B is along +y), we find that the magnetic force points upwards along the positive z-axis. Calculating its magnitude qvB, we discover something remarkable: it is exactly 1.6384×10−14 N!
The electric and magnetic forces are perfectly balanced. They are equal in magnitude but opposite in direction, resulting in a net force of zero.
The Journey to Point P
Because the net force is zero, the particle experiences no acceleration. It continues to move in a straight line along the x-axis with its initial constant velocity.
We are asked to find its position at t1=5×10−6 s. Using the simple kinematic equation for constant velocity, x=vt, we find:
x=(1.28×106 m/s)×(5×10−6 s)=6.4 m
At this moment, the particle is at point P(6.4,0,0).
A Sudden Change
Circular Motion Begins
At exactly t=5×10−6 s, the electric field is abruptly switched off. The delicate balance is broken! The particle is now solely under the influence of the magnetic field.
Since the particle's velocity is perpendicular to the uniform magnetic field, it will immediately begin to move in a circular path. Because the velocity is along the x-axis and the magnetic field is along the y-axis, the magnetic force (and thus the circular path) will lie entirely in the x-z plane.
Let's determine the parameters of this circular motion. The radius r is given by:
r=qBmv=(1.6×10−19)(8×10−2)(10−26)(1.28×106)=1 m
The angular velocity ω is:
Tracing the Semi-Circle
The particle travels in this circular path for the remaining time interval, Δt=7.45×10−6 s−5×10−6 s=2.45×10−6 s.
How much of the circle does it trace in this time? We calculate the angle rotated, θ:
θ=ωΔt=(1.28×106)×(2.45×10−6)=3.136 rad
Notice that 3.136 is approximately equal to π radians (180∘). This means the particle completes exactly a semi-circle!
Starting from point P(6.4,0,0), it swings through the x-z plane. After a full semi-circle, its x-coordinate returns to 6.4 m, its y-coordinate remains 0, and its z-coordinate increases by the diameter of the circle (2r=2 m).
Therefore, the final position of the particle is Q(6.4,0,2).