(D'arsonval galvanometer) moving coil meter

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SUMMARY

The discussion centers on the operational principles of the d'Arsonval galvanometer, a type of moving coil meter. It highlights the relationship between the current (I) in the coil and the angle (φ) of the coil in a magnetic field, expressed by the formula I = (c/BA)(φ/cos(φ)). The non-linear behavior of current as a function of angle is emphasized, particularly in the context of the non-uniform magnetic field created by the iron core. The equilibrium condition is established when the magnetic torque (τ_M) equals the mechanical torque of the torsional spring, leading to a calibrated scale based on known currents.

PREREQUISITES
  • Understanding of magnetic fields and torque in physics
  • Familiarity with the principles of electromagnetism
  • Knowledge of moving coil meter operation
  • Basic grasp of torque equilibrium concepts
NEXT STEPS
  • Study the principles of magnetic dipoles and their interactions with magnetic fields
  • Explore the calibration techniques for moving coil meters
  • Learn about the effects of non-uniform magnetic fields on coil behavior
  • Investigate the design and applications of d'Arsonval galvanometers in measurement systems
USEFUL FOR

Physics students, electrical engineers, and professionals involved in instrumentation and measurement who seek to understand the mechanics of moving coil meters and their applications in various fields.

Siune
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Hello, just been reading a little bit about the basics of moving coil meter and one thing is bugging me.

First if we have a basic square looped coil in and uniform magnetic field. There is torque ( m x B ) due to the magnetic field and then there is the system/spring attached to the coil which gives the opposing torque ( cθ ).

So in the end we get that the current in the coil is:

I = \frac{c}{BA} \frac{\phi}{cos(\phi)}

Cleary the I is very non-linear as function of phi as the surface of the coil makes angle with the magnetic field ( Which is uniform ).

Now we have d'Arsonval galvanometer, like in the picture:

180px-Galvanometer_diagram.png


Now the magnetic field is clearly not uniform as the "iron core" sucks in the magnetic field. The field between the poles and the iron core becomes radial. Now it says that the surface area vector of the plane of the loop (n or m if we talk about dipole ) is always perpendicular to the magnetic field. I can't really figure it out as the magnetic field inside is uniform ( horizontal ) inside the soft iron core.

I can understand that the coil is wounded around the iron core so we should compare the field to the outside field ( radial ) but as we compare the angle with the normal vector of the surface of the loop and the magnetic field so. :l


The page is 424, in Understanding Physics, Mansfield & O'Sullivan (Second edition).
http://books.google.fi/books?id=19TCz0cxAFMC&printsec=frontcover&hl=fi#v=onepage&q&f=false
 
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Think of the current in the red coil generating a magnetic dipole ##\mu##. The magnitude of this dipole is proportional to the current ##I##. The external field due to the poles of the permanent magnet exerts a magnetic torque against the mechanical torque of the torsional spring that is attached to the needle. When the two opposing torques have equal magnitudes (##\tau_M=\tau_{spring}##, the needle is in equilibrium. Now ##\tau_M=\mu B\sin\theta## where ##\theta## is the angle between the dipole and the magnetic field. By setting the torques equal, you see that a given angle of equilibrium corresponds to a given current. The scale is calibrated by sending known currents in the meter.
 

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