Energy imparted to an ion by a magnetic field

In summary, the conversation discusses the relationship between an anion and a magnet, and whether there is a force or energy imparted on the anion when placed near the negative pole of a magnet. It is determined that magnets do not have negative poles and therefore do not interact with charged particles. The concept of Coulomb's law is mentioned as a potential calculation for force, but it does not directly relate to kinetic energy. Overall, it is concluded that there is no force on the anion when placed near a magnet, unless the anion is in motion.
  • #1
Ken H
2
0
Basically my question is: if an anion is placed by the negative poll of a magnet will it push on the particle?
 
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  • #2
Negative charges repel negative charges, and positive charges repel positive charges.
 
  • #3
Is there a calculation for the amount of kinetic energy imparted to the particle? Also where does the power come from, is the strength of the magnetic field reduced?
 
  • #4
Ken H said:
Is there a calculation for the amount of kinetic energy imparted to the particle?
Perhaps Coulomb's law? I'm no master of electromagnetism but it seems like the equation would apply in this case.
 
  • #5
Coulomb's law would give you the force, though, and not kinetic energy. You would have to use other equations to find the kinetic energy.
 
  • #6
Ken H said:
Basically my question is: if an anion is placed by the negative poll of a magnet will it push on the particle?
No. The poles of a magnet are not charged.
 
  • #7
Dale said:
No. The poles of a magnet are not charged.
If it is just a negative pole in general it would still repel the anion though, correct?
 
  • #8
Magnets don't have negative poles. They have north and south poles.
 
  • #9
Dale said:
Magnets don't have negative poles. They have north and south poles.
I don't know why I used poles in that. I just meant a negative charge.
 
  • #10
Yes, an anion is negatively charged so it will be repelled from other negative charges. This has nothing to do with a magnet since magnets are typically uncharged.
 
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  • #11
Going back to the original question, if you "place" a charge near the pole of a magnet, and if the word "place" means the charge is not moving when you place it, then, as Dale stated above, there is no force on the charge. If the charge has a velocity, there is a force on the charge depending on the direction of the velocity and the magnetic field.
 
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FAQ: Energy imparted to an ion by a magnetic field

What is energy imparted to an ion by a magnetic field?

Energy imparted to an ion by a magnetic field refers to the amount of energy that is transferred to an ion as it moves through a magnetic field. This energy can affect the ion's motion, speed, and direction.

How is energy imparted to an ion by a magnetic field calculated?

The energy imparted to an ion by a magnetic field is calculated using the formula E = qVB, where E is the energy, q is the charge of the ion, V is the velocity of the ion, and B is the strength of the magnetic field.

What factors affect the amount of energy imparted to an ion by a magnetic field?

The amount of energy imparted to an ion by a magnetic field is affected by the strength of the magnetic field, the velocity of the ion, and the charge of the ion. A stronger magnetic field or a higher velocity will result in more energy being imparted to the ion.

How does energy imparted to an ion by a magnetic field affect the ion's trajectory?

The energy imparted to an ion by a magnetic field can change the direction of the ion's motion, causing it to deviate from its original path. This is because the ion experiences a force from the magnetic field that alters its trajectory.

What are some practical applications of energy imparted to an ion by a magnetic field?

This phenomenon is utilized in a variety of technologies, such as particle accelerators, mass spectrometers, and magnetic resonance imaging (MRI) machines. It is also important in understanding the behavior of charged particles in space and in the Earth's magnetic field.

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