A charged particle moves with a uniform velocity 4a_{x}m/s in a region where E=20a_{y}V/m and B=B_{o}a_{z}Wb/m^{2}. Determine B_{o} such that the velocity of the particle remains constant.
A charged particle moves with a uniform velocity 4a_{x}m/s in a region where E=20a_{y}V/m and B=B_{o}a_{z}Wb/m^{2}. Determine B_{o} such that the velocity of the particle remains constant.
If the particle moves with a constant velocity, it is implied that its acceleration is zero. In other words, the particle experiences no net force. Hence
0=F=ma=Q(E+u\times B)
0=Q(20a_{y}+4a_{x}\times B_{o}a_{z})
or
-20a_{y}=-4B_{o}a_{y}
Thus B_{o}=5.
This example illustrates an important principle employed in a velocity filter shown in Figure 8.3. In this application, E, B, and u are mutually perpendicular so that Qu\times B is directed opposite to QE, regardless of the sign of the charge. When the magnitudes of the two vectors are equal
QuB=QE
or
u=\frac{E}{B}
This is the required (critical) speed to balance out the two parts of the Lorentz force. Particles with this speed are undeflected by the fields; they are “filtered” through the aperture. Particles with other speeds are deflected down or up, depending on whether their speeds are greater or less than this critical speed.