Magnetic field of circular loop

In summary, two small identical circular loops carrying equal currents and placed perpendicular to each other produce a magnetic field of magnitude μIR^2/2x^3 at a point O at a distance x from their centers. The fields are perpendicular and inclined at a 45° angle with the horizontal. The direction of the field may vary depending on the direction of current flow, which cannot be determined from the information given.
  • #1
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Homework Statement


Two small identical circular loops carrying equal currents are placed with the geometrical axis perpendicular to each other. Find the magnitude and direction at a point O at an equal distance x from their centers.

Homework Equations


Magnetic field of a current carrying circular loop at a distance x on it's axis : μIR2/2x3 when x>>>R

The Attempt at a Solution


Let μIR2/2x3 = B
Then magnitude should be (21/2)B(Fields perpendicular to each other)
Inclined at an angle 45° with the horizontal.

Are my directions right?
 

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  • #2
Your equation for the magnetic field seems like it's missing a factor of 2 in the denominator. Also, check your vector addition when adding the magnitudes of the fields.
 
  • #3
Directions look right, although, it's hard for the viewer to be certain of the direction of current flow.

B1/2 is not correct. That's the square root of B.
 
  • #4
!
Sorry about that. I meant, (21/2)B (I don't know how to make the squareroot symbol here) And yes, the equation was missing a 2. Typo again.
I don't have any problems with the magnitude. Just the direction. The solution in my book has a direction opposite to the one I got.
 
  • #5


Your directions are not quite right. The correct directions would be:

- The magnitude of the magnetic field at point O is given by B = μIR^2 / 2x^3, where R is the radius of the circular loops and x is the distance from their centers.
- The direction of the magnetic field at point O would depend on the direction of the currents in the loops. If the currents are in the same direction, the magnetic field would be pointing out of the page (perpendicular to the plane of the loops). If the currents are in opposite directions, the magnetic field would be pointing into the page (perpendicular to the plane of the loops).
- The magnetic fields from the two loops would combine at point O, resulting in a net magnetic field that is inclined at an angle of 45° with the horizontal.
 

Related to Magnetic field of circular loop

What is the definition of a magnetic field?

A magnetic field is a physical phenomenon created by moving electric charges, which exerts a force on other moving charges. It is represented by lines of force that form loops around the magnetic source.

How is a magnetic field created in a circular loop?

A magnetic field is created in a circular loop when an electric current flows through the loop. The current creates a magnetic field that is perpendicular to the plane of the loop, and the strength of the field is directly proportional to the amount of current flowing through the loop.

What is the direction of the magnetic field in a circular loop?

The direction of the magnetic field in a circular loop is determined by the direction of the electric current flowing through the loop. The field lines flow in a counterclockwise direction when viewed from above the loop if the current is flowing counterclockwise, and in a clockwise direction if the current is flowing clockwise.

How does the radius of a circular loop affect its magnetic field?

The radius of a circular loop has a direct effect on the strength of its magnetic field. The greater the radius, the larger the area encompassed by the loop and the stronger the magnetic field. This is because the magnetic field lines are more spread out in a larger loop, resulting in a weaker field in each individual line.

What are some practical applications of the magnetic field of a circular loop?

The magnetic field of a circular loop has many practical applications, including in electric motors, generators, and transformers. It is also used in magnetic compasses, MRI machines, and particle accelerators. The field can also be manipulated to produce magnetic levitation, as seen in Maglev trains.

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