Stern-Gerlack Experiment with silver atoms

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SUMMARY

The Stern-Gerlach experiment with silver atoms involves a magnetic field that increases by 26.00 T per centimeter, with a magnet length of 7.1 cm and silver atom speed of 922 m/s. The force acting on the silver atoms is defined by F = -∇V and F_z = -m_l μ_B (dB_z/dz). The separation of the two silver atom beams can be calculated using these parameters, taking into account the mass of the silver atom, which is 1.800×10-25 kg. The discussion highlights the need to consider multiple angular momentum states and the relationship between force and acceleration in this context.

PREREQUISITES
  • Understanding of the Stern-Gerlach experiment principles
  • Familiarity with magnetic fields and their gradients
  • Knowledge of classical mechanics, particularly Newton's laws
  • Basic quantum mechanics concepts, especially angular momentum
NEXT STEPS
  • Calculate the force on silver atoms in varying magnetic fields
  • Explore the implications of angular momentum states in quantum mechanics
  • Learn about the mathematical derivation of beam separation in Stern-Gerlach experiments
  • Investigate the role of atomic mass in magnetic field interactions
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Physics students, educators, and researchers interested in quantum mechanics and experimental physics, particularly those studying atomic behavior in magnetic fields.

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Homework Statement



The magnetic field in a Stern-Gerlach experiment varies along the vertical direction so that the magnetic field increases by 26.00 T each centimeter. The horizontal length of the magnet is 7.1 cm, and the speed of the silver atoms is 922 m/s. The mass of the silver atom is 1.800×10-25 kg. What is the separation of the two silver atom beams as they leave the magnet?

Homework Equations



[itex]F = - \nabla V[/itex]

[itex]F_{z} = - m_{l} \mu_{B} \frac{dB_z}{dz}[/itex]

[itex]B = 2600 z[/itex]

where z is the vertical position

The Attempt at a Solution



I started out thinking I was looking for an angle between the two paths, so I found

F = -2600

and [itex]F_z = - \mu_B (2600)[/itex]

solving for theta:

[itex]\theta = tan^{-1}(\frac{-2600\mu_{B}}{-2600})[/itex]

which simplifies to [itex]tan^{-1}(\mu_B)[/itex]

and that doesn't sit well with me.

Any ideas?
 
Last edited:
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and that doesn't sit well with me.
why not?

why do you have a F as well as Fz?
how did you use the length of the magnet and the speed of the atoms?
did you take into account that there is more than one angular momentum state involved?

note:
##F_z = m_{Ag}a_z## isn't it?
 

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