Magnetic image of a coil over a conducting surface

In summary: This is because the image current produces its own magnetic field, which acts in the opposite direction of the coil's magnetic field.
  • #1
mkarabiyik
1
0

Homework Statement



If the coil in the figure is touching to an ideally conducting (σ=∞) non-magnetic steel from the A4-A5 side, what would be the magnetic field in the gap. Assume A1=A2=A3=A4=A5.

Homework Equations



220px-Magnetischer_Kreis.svg.png



The Attempt at a Solution



I have calculated that when the coil is alone, the magnetic field in the gap is

B=μ0NI/g
where g is the gap at A5

So how the results modifies when there is an image coil induced by the conducting metal.
Thanks
 
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  • #2
for your post, I appreciate your question.

When a conducting metal is placed near a coil, it can induce an image current in the metal. This image current produces its own magnetic field, which can affect the overall magnetic field in the gap of the coil. In this case, since the metal is ideally conducting, the image current will be equal in magnitude and opposite in direction to the current in the coil. This means that the total magnetic field in the gap will be the sum of the magnetic fields produced by the coil and the image current.

To calculate the magnetic field in the gap, you can use the superposition principle, which states that the total field is equal to the sum of the individual fields. In this case, the magnetic field in the gap can be calculated as:

B_total = B_coil + B_image

where B_coil is the magnetic field produced by the coil alone and B_image is the magnetic field produced by the image current.

Since the coil and the image current are equal in magnitude and opposite in direction, their magnetic fields will cancel each other out. This means that the net magnetic field in the gap will be zero.

In summary, when a conducting metal is placed near a coil, the presence of the image current will cancel out the magnetic field in the gap, resulting in a net magnetic field of zero.
 

FAQ: Magnetic image of a coil over a conducting surface

Q1: What is a magnetic image of a coil over a conducting surface?

A magnetic image of a coil over a conducting surface is a phenomenon that occurs when a coil carrying an electric current is placed above a conducting surface. The current in the coil creates a magnetic field, which induces an opposite magnetic field in the conducting surface. This results in a mirrored or "image" magnetic field below the surface that interacts with the original field to produce a combined field.

Q2: How is the magnetic image affected by the properties of the conducting surface?

The properties of the conducting surface, such as its electrical conductivity and thickness, can affect the strength and distribution of the magnetic image. A highly conductive surface will have a stronger magnetic image compared to a less conductive surface. A thicker surface may also result in a weaker magnetic image due to increased resistance to the induced magnetic field.

Q3: What are some applications of the magnetic image of a coil over a conducting surface?

The magnetic image phenomenon has various applications in industries such as non-destructive testing, metal detection, and electromagnetics. It is also utilized in devices such as metal detectors, magnetic sensors, and proximity sensors.

Q4: How is the magnetic image of a coil calculated?

The magnetic image can be calculated using mathematical formulas that take into account the properties of the coil, the conducting surface, and the distance between them. These calculations can be complex and may require the use of specialized software or tools.

Q5: Can the magnetic image be manipulated or controlled?

Yes, the magnetic image can be manipulated by changing the properties of either the coil or the conducting surface. For example, the strength of the magnetic image can be increased by using a more powerful current in the coil or by increasing the conductivity of the surface. The distance between the coil and the surface can also be adjusted to control the distribution of the magnetic image.

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