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  • Operation of a mass spectrometer.

  • Lorentz force.

  • Radial (centripetal) force

Topics:  Lorentz force, electromagnetism, radial (centripetal) force, mass spectroscopy.

Pre-requisite skills:  Elementary understanding of basic electrostatics and Newton's Second Law.

Approximate completion time:  Under an hour.

Provide sufficient detail to verify that the assignment was completed in a meaningful manner.

MERLOT site:   Mass Spectrometer, by Larry Gladney.  (direct link).

Applet by Larry Gladney

1.  Familiarize yourself with the operation of the applet. There are three buttons on the right side of the applet that are particularly important -- "Start," "Stop," and "Reset."  To change a value of a parameter, the applet must first be stopped by pressing "Stop."  Then after changing the parameter press the "Start" button. The "Reset" button will activate the applet and show a particle traveling through an external magnetic field.  In other words, to change a parameter the following sequence of operations must be performed:   (a) "Stop," (b) change parameter, (c) "Start," (d) "Reset."

Upon loading the site the following values for the parameters should be preset.  (See Table I.)   If this is not the case, make the necessary changes.

Table I.  Initial Values of Physical Parameters.

q

v

B

m

+1

5 X 107 m/s

0.5 T

+1

(a) Adjust the field strength B such that the particle hits closest to the left-upper corner of the shaded-purple area.  What field strength does this correspond?

(b) Why does the radius of curvature shorten when the field is increased in strength? (Explain in terms of the net force acting on the particle.)

(c)  Now increase the speed of the charged particle to v = 10 X 107 m/s.  Explain what happens to the radius of curvature of the charged particle.   What value of field strength will produe the same radius of motion as found in part (a)?  (Show all work.)   Does the operation of the applet verify your calculations?


2. Reset all physical variables to coincide with those listed in Table I and run the applet.  Now change the charge q on the particle from +1 to -1 and run the applet again. 

(a) Describe how the path of the charged particle changes.

(b) If the charge on the object was doubled (from -1 to -2), what would happen to the radius of curvature?   Calculate the change in this radius from Newton's Second Law.  

(c) Does the operation of the applet verify your calculations?

(d)  Describe, in terms of the net force acting on the particle, why you would expect such a result from inreasing the charge on the particle.


3.  Again, reset all physical variables to those listed in Table I and run the applet.  Now double the mass of the particle and run the applet.

(a)  Describe the change in the radius of curvature.   Calculate the change in this radius from Newton's Second Law. Does the operation of the applet verify your calculations? 

(b) Describe qualitatively why you would expect such a change in the motion by increasing the mass of the particle.


4.  Again, reset all physical variables to those listed in Table I and run the applet.   Now press the "Reverse B" button.  Notice that the field direction is now pointing into the page (away from you).  Run the applet again and describe what changes in the motion of the charged particle.  What does not change?

5.  For a given motion (that is, a motion defined by the direction -- clockwise or counter-clockwise -- and radius of curvature) describe five ways that the physical properties of the system can be changed yet produce the exact same motion.   Limit your changes to situations where physical properties are doubled or halved.  Do not forget that the field can be reversed in direction.  To ensure correctness, use the applet to verify your answers.

Helpful Resources

  1. Mass Spectrometer by Angel Franco Garcia..
  2. Mass Spectrometer by Tony Abou-Assaleh.
  3. Charged Particle Motion in E/M Field by Fu Kwun Hwang.
  4. Motion in an Electromagnetic Field by Mark Sutherland.
  5. Charged Particles Moving in a Magnetic Field by Sergey Kiselev

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