Calculate Magnetic Force on Iron: B0 & Cylinder

Click For Summary

Discussion Overview

The discussion revolves around calculating the magnetic force experienced by a cylindrical piece of iron placed near a solenoid with a specified internal magnetic field strength (B0). Participants explore the relationship between magnetic field strength, its gradient, and the energy stored in the system, examining both theoretical and practical aspects of the problem.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant inquires about the calculation of the force on a cylindrical piece of iron near a solenoid, emphasizing the need for clarity on the dependence of force on magnetic field strength.
  • Another participant asserts that the force is dependent on the gradient of the magnetic field rather than the field strength itself, noting that this gradient is zero for an ideal solenoid.
  • A participant suggests calculating the force by examining changes in the total stored magnetic energy as the iron object is displaced, proposing the relationship Fx = dW/dx.
  • There is a discussion on the energy density of the magnetic field inside and outside the iron, with one participant arguing that energy stored inside the iron increases as it moves closer to the solenoid, while another counters that the energy density is actually higher in the surrounding air.
  • Participants explore the implications of the continuity of the magnetic field components at the air/iron interface, with conflicting views on how this affects energy storage and the resulting forces.
  • Questions arise regarding whether it is the magnetic field (B) or the magnetic field strength (H) that remains continuous across the air and iron interface, indicating uncertainty in the definitions used.

Areas of Agreement / Disagreement

Participants express differing views on the relationship between magnetic energy storage and the force experienced by the iron piece. There is no consensus on whether the energy stored in the iron increases or decreases as it approaches the solenoid, leading to conflicting interpretations of the magnetic force acting on the iron.

Contextual Notes

Participants reference specific equations and concepts related to magnetic energy density and the behavior of magnetic fields in different materials, but there are unresolved assumptions regarding the ideal versus real solenoid conditions and the implications of energy continuity at material boundaries.

I_am_learning
Messages
681
Reaction score
16
I searched different places but couldn't find how actually you calculate this:-
What is the magnitude of force experienced by a cylindrical piece of iron placed near the end of a solenoid with internal field strength B0.
 
Physics news on Phys.org
The reason you keep asking this and not getting an answer is that the force is not dependent on the field strength. It's dependent on the gradient of the field strength. This is zero for an ideal (long) solenoid and complicated for a real one.
 
Vanadium 50 said:
It's dependent on the gradient of the field strength.
Ok, then how do i calculate the force if I know the gradient of the field i.e. I know the function B(x,y,z).
 
thecritic said:
Ok, then how do i calculate the force if I know the gradient of the field i.e. I know the function B(x,y,z).
One way to calculate the force is to examine how the total stored magnetic energy W of the system changes if the iron object is displaced by a distance dx. As you know, work (energy) is force F times distance dx. So the derivative of the stored energy W in the direction dx is the force in the direction dx:

Fx = dW/dx.

Smythe's (Static and Dynamic Electricity) exact solution for the axial field of a finite length solenoid is given in post #4 (see thumbnail) of this thread:
https://www.physicsforums.com/showthread.php?t=352947

Bob S
 
Last edited:
Bob S said:
Thanks for that. It really helped me.

Bob S said:
One way to calculate the force is to examine how the total stored magnetic energy W of the system changes if the iron object is displaced by a distance dx. As you know, work (energy) is force F times distance dx. So the derivative of the stored energy W in the direction dx is the force in the direction dx:
Fx = dW/dx.
So can I proceed like this to calculate the force on a small iron piece lying some distance from the axis of the solenoid.?
1. The B inside the iron is multiplied by factor ur, So Biron=urBu0
2.The total Energy stored inside the piece can be calculated by intergrating over the entire volume of the iron piece
http://hyperphysics.phy-astr.gsu.edu/%E2%80%8Chbase/electric/imgele/engbf.gif
3. When the iron piece is moved a small distance then then the total Energy Stored will change.

Then applying Fx = dW/dx. will give the force.
 
Last edited by a moderator:
I believe the magnetic energy density outside the iron is

(1/2μ0)∫B2 dV

and inside the iron it is

(1/2μμ0)∫B2 dV

so because B is continuous there is very little energy stored inside the iron.

But there is a dipole field outside the iron that I have not included.

I know there is a thread on this but I cannot find it.

Bob S
 
Bob S said:
Inside the iron it is
(1/2μμ0)∫B2 dV
so because B is continuous there is very little energy stored inside the iron.
on the contrarary I think there is lot of energy inside the iron because
the total energy inside iron, as you pointed out, is
(1/2μμ0)∫B2 dV
But, B = μB0
So, the energy stored becomes
(1/2μμ0)∫(Bμ)2 dV
= (1/2μμ02∫B2 dV
= (μ/2μ0)∫B2 dV

When the piece of iron is moved a small distance towards the solenoid, the intensity of B increases, so does the energy stored inside the iron.
So, the iron shouldn't move towards the solenoid (since it creates increased energy).
This is directly against the fact that the iron piece is attracted towards the solenoid!??
 
Last edited:
thecritic said:
on the contrarary I think there is lot of energy inside the iron because
the total energy inside iron, as you pointed out, is
(1/2μμ0)∫B2 dV
But, B = μB0
So, the energy stored becomes
(1/2μμ0)∫(Bμ)2 dV
= (1/2μμ02∫B2 dV
= (μ/2μ0)∫B2 dV

When the piece of iron is moved a small distance towards the solenoid, the intensity of B increases, so does the energy stored inside the iron.
So, the iron shouldn't move towards the solenoid (since it creates increased energy).
This is directly against the fact that the iron piece is attracted towards the solenoid!??
Err... no. Very little energy is stored in the iron. Because the normal component of B is continuous, the energy density is higher in the air than in the iron. See thumbnail.
Bob S
 

Attachments

  • Magnet_air_gap.jpg
    Magnet_air_gap.jpg
    38.2 KB · Views: 2,438
Last edited:
Bob S said:
Err... no. Very little energy is stored in the iron. Because the normal component of B is continuous, the energy density is higher in the air than in the iron.
Bob S
But In wikipaedia I read this:
f0d14e04603d965b4d625a59745dae55.png

(here u is the total energy stored).
I am confused that, Is it B or H , that is same for both air core and iron-core solenoid?
 
  • #10
The basic form for the energy stored in a magnetic field is

W = (1/2)∫ B H dV

In a magnetic system that has both iron and air in the same flux, only B (the normal component) is continuous at the air / iron interface. So we write

W = (1/2μrμ0)∫ B2 dV in iron, and

W = (1/2μ0)∫ B2 dV in air

Bob S
 

Similar threads

  • · Replies 21 ·
Replies
21
Views
4K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 27 ·
Replies
27
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 8 ·
Replies
8
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K