Faraday Rotation Effect Lab -- sources of components....

AI Thread Summary
The discussion focuses on assembling a Faraday Rotation Effect Lab, with participants sharing resources and calculations related to solenoids and magnets. A link to a field strength calculator is appreciated, and recommendations for lab supply companies offering solenoids capable of 0.5T or higher are sought. Detailed calculations reveal the challenges of generating a 0.5T magnetic field, highlighting the significant number of wire turns and the required wire specifications to manage heat dissipation. The feasibility of using short pulses and integrated cooling for higher power dissipation is mentioned, along with the potential of superconducting coils, albeit at a high cost. Overall, the conversation emphasizes the technical complexities and resource needs for the lab setup.
Dan LaSota
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I appreciate the link to the field strength calculator. http://www.calctool.org/CALC/phys/electromagnetism/solenoid
I'm also looking for recommendations on sources for magnets. What I'm trying to do is put together a Faraday Rotation Effect Lab.

This is my Faraday Rotator, a 12 cm x 2.0 cm cylinder of something close to flint glass with a half decent Verdet Constant.
IMG_1701.jpg


Does anyone have pointers to a lab supply company with solenoids capable of 0.5T or higher?
 
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Not really my subject but I think it would be difficult to generate a field of 0.5T in that tube. For example at 1A I calculated you would need 95,400 turns of wire. At 100A it's 954 turns.
 
400 kA/m assuming µr of about 1, with a length of 12 cm we need 50 kA ring current.

Let's check 5000 turns at 10 A: With 2 cm diameter, the wire has a length of 314 meters. To limit heat dissipation to 100 W with copper, voltage has to be 10 V, which means 1 Ohm resistance, which needs 5 mm^2 wire cross section. At 2.5 mm between adjacent windings, only 48 windings fit next to each other, so you need 100 layers which makes the coil 25cm thick (in radius). Uhm...
The 10 A were arbitrary, but the conclusion doesn't change if we plug in other values: Double it and you half the voltage, which leads to 1/4 the resistance at 1/2 the total length, so cross-section goes up by a factor 2 and we arrive at the same thickness again.

Very short pulses would allow a higher power dissipation, integrated cooling helps as well. Superconducting coils can easily provide such a magnetic field. All those solutions exist commercially, but they are quite expensive.
 
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