Circular Motion in a Simple Mass Spectrometer

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SUMMARY

The discussion focuses on calculating the magnitude and direction of the magnetic field (B) in a simple mass spectrometer, where positive ions are accelerated through a potential difference (ΔV) before entering a magnetic field. The relevant equations include the magnetic force equation (Fmag = qvB) and the kinetic energy equation (mv² = 2qΔV). The correct expression for the magnetic field is derived as B = 2Mv/dq, where M is the mass of the ion, q is its charge, and d is the distance between the accelerating plates. The challenge lies in determining the velocity of the ions, which is linked to the potential difference through the kinetic energy equation.

PREREQUISITES
  • Understanding of basic physics concepts, particularly electromagnetism.
  • Familiarity with the equations of motion and energy conservation.
  • Knowledge of mass spectrometry principles.
  • Ability to manipulate algebraic equations involving variables such as mass, charge, and potential difference.
NEXT STEPS
  • Study the relationship between electric potential and kinetic energy in charged particles.
  • Learn how to derive the velocity of charged particles in electric fields using the equation v = sqrt(2qΔV/m).
  • Explore the principles of magnetic fields and their effects on charged particles in motion.
  • Investigate the design and function of mass spectrometers, focusing on the role of magnetic fields.
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Students studying physics, particularly those focusing on electromagnetism and mass spectrometry, as well as educators seeking to explain the principles of charged particle motion in electric and magnetic fields.

Oribe Yasuna
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Homework Statement


In the simple mass spectrometer shown in the figure below, positive ions are generated in the ion source. They are released, traveling at very low speed, into the region between two accelerating plates between which there is a potential difference ΔV. In the shaded region there is a uniform magnetic field B
rightarrowhead.gif
; outside this region there is negligible magnetic field. The semicircle traces the path of one singly charged positive ion of mass M, which travels through the accelerating plates into the magnetic field region, and hits the ion detector as shown.

Determine the appropriate magnitude and direction of the magnetic field B
rightarrowhead.gif
, in terms of the known quantities shown in the figure below (in addition to M and q, where q is the charge on an ion).

Magnitude B = ?
direction = ?

14f06f7925.png


Homework Equations


Fmag = dp/dtmag = qvB
dp/dtmag = p(v/R) = p(omega), p = ymv
omega = q_mag * b / (ym)

The Attempt at a Solution


deltaV (I don't know what to do with electrical potential)
M (mass)
q (charge)
d/2 = R (radius)
v << c, y = 1, p = mv (approximation)

Fmag = dp/dtmag
qvB = p(v/R)
qvB = p(v/(d/2))
qB = p/(d/2))
B = p/(d/2))/q
B = 2p/dq, p = mv (approx.)
B = 2Mv/dq

This is wrong, probably because I'm not given velocity. However, I don't know how to get magnetic field without velocity? I think the problem is I don't know what to do with electric potential.
 
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Your ion with charge q is accelerating through the ΔV between the plates. Look for an equation relating the energy acquired by an electric charge accelerating through a potential difference.
 
1/2 mv^2 = q deltaV

This kinetic energy equation?

mv^2 = 2q deltaV
v^2 = 2q deltaV / m
v = sqr rt (2q delta V / m)
 
deltaV = Ed

But I'm missing both E and d? d is the separation between the plates but the variable d in the image seems to be a length.
 
Oribe Yasuna said:
deltaV = Ed

But I'm missing both E and d? d is the separation between the plates but the variable d in the image seems to be a length.
There's another equation that involves the charge.
 

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