Stern Gerlach Gradient Field Strength

In summary, the conversation discusses the difficulty in calculating the gradient magnetic field for recreating the Stern-Gerlach experiment. It is suggested to use the gradient of the inproduct of the magnetic moment and the magnetic field, and to consider each volume of magnetic material as a point dipole field. Integration can be used to derive the total magnetic field.
  • #1
rwhitman
1
0
I am trying to recreate the Stern-Gerlach experiment and am having trouble trying to calculate the gradient magnetic field. I am using two magnets with one having a sharp edge and the other flat. I have calculated what the deflection will be of the electron will be in terms of the gradient field, but I do not know how to calculate what the gradient is knowing the dimensions of the magnets.

~Robert
 
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  • #2
Make sure you use the gradient of the inproduct of the magnetic moment and the
magnetic field rather than the gradient of the magnetic field itself.

[tex]\vec{F}_{magn}\ =\ \textsf{grad}\left( \vec{\mu}_e\cdot
\textsf{B} \right)[/tex]

What you could do is assuming that every little volume of magnetic material is a
point dipole field like this:

[tex]\textsf{B}~ = ~ \ \frac{\mu_o\mu_e}{4\pi r^3}\ \ \left(\ 3\ \frac{xz}{r^2}, \quad 3\ \frac{yz}{r^2}, \quad 3\ \frac{zz}{r^2}-1\ \right)[/tex]

Assuming that they all point in the same direction you can derive the total
magnetic field by integration (analytic or numerical)Regards, Hans.
 
Last edited:
  • #3


Hello Robert,

Thank you for sharing your interest in recreating the Stern-Gerlach experiment. The gradient magnetic field strength can be calculated using the formula:

B = μ0 * (m1-m2) / (2 * d)

where B is the magnetic field strength, μ0 is the permeability of free space (4π*10^-7 T*m/A), m1 is the magnetic moment of the sharp-edge magnet, m2 is the magnetic moment of the flat magnet, and d is the distance between the two magnets.

To calculate the magnetic moment of the magnets, you can use the formula:

m = m0 * A * n,

where m0 is the magnetic moment per unit volume, A is the cross-sectional area of the magnet, and n is the number of magnetic domains in the magnet.

Once you have calculated the magnetic field strength using the first formula, you can use this value to determine the deflection of the electron in terms of the gradient field.

I hope this helps and good luck with your experiment! If you have any further questions, please don't hesitate to ask.

 

1. What is the Stern Gerlach gradient field strength?

The Stern Gerlach gradient field strength is a measure of the strength of the magnetic field gradient in the Stern Gerlach experiment. It refers to the change in magnetic field strength over a certain distance.

2. How is the Stern Gerlach gradient field strength measured?

The Stern Gerlach gradient field strength can be measured using a variety of techniques, such as using a gaussmeter or a Hall probe. These instruments can detect the magnetic field strength at different points in the gradient and calculate the gradient field strength.

3. What is the importance of the Stern Gerlach gradient field strength?

The Stern Gerlach gradient field strength is important because it determines the amount of deflection that a beam of particles will experience in the Stern Gerlach experiment. It is also a crucial parameter in understanding the behavior of quantum particles in a magnetic field gradient.

4. How does the Stern Gerlach gradient field strength affect the outcome of the experiment?

The Stern Gerlach gradient field strength directly affects the amount of deflection of the particles in the experiment. A stronger gradient field will result in a larger deflection, while a weaker gradient field will result in a smaller deflection. This ultimately determines the outcome of the experiment and the behavior of the particles.

5. Can the Stern Gerlach gradient field strength be controlled?

Yes, the Stern Gerlach gradient field strength can be controlled by adjusting the magnetic field strength and the distance between the magnets in the experiment. This allows for precise manipulation of the particles and their behavior in the experiment.

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