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Field and flux of a magnetic dipole. The magnetic field at a point M(r, θ) distant from a magnetic dipole m is expressed as B(M) = − µ0 4π ∇ m · r r 3  This formula is identical to that of the electric field produced by an electric dipole moment m, after changing µ0 into 1/0. q m i z r ur uq O O’ M a R’ We consider a small planar and circular loop of center O, radius a, carrying a current i and we use a spherical coordinate system (r, θ, ϕ) with the z-axis oriented along the magnetic dipole moment: m = muz. The expression of the gradient in spherical coordinates is as follow: ∇φ = ∂φ ∂r ur + 1 r ∂φ ∂θ uθ + 1 r sin θ ∂φ ∂ϕuϕ a. Express the corresponding magnetic dipole moment as a function of a and i.

Question

Field and flux of a magnetic dipole. The magnetic field at a point M(r, θ) distant from a magnetic dipole m is expressed as B(M) = − µ0 4π ∇ m · r r 3  This formula is identical to that of the electric field produced by an electric dipole moment m, after changing µ0 into 1/0. q m i z r ur uq O O’ M a R’ We consider a small planar and circular loop of center O, radius a, carrying a current i and we use a spherical coordinate system (r, θ, ϕ) with the z-axis oriented along the magnetic dipole moment: m = muz. The expression of the gradient in spherical coordinates is as follow: ∇φ = ∂φ ∂r ur + 1 r ∂φ ∂θ uθ + 1 r sin θ ∂φ ∂ϕuϕ a. Express the corresponding magnetic dipole moment as a function of a and i.

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Solution

The magnetic dipole moment (m) of a small planar and circular loop of current is given by the product of the current (i) and the area (A) of the loop.

For a circular loop, the area (A) is given by πa², where a is the radius of the loop.

Therefore, the magnetic dipole moment (m) can be expressed as a function of the current (i) and the radius (a) of the loop as follows:

m = i * πa²

This is the magnetic dipole moment as a function of a and i.

This problem has been solved

Similar Questions

Time left 0:01:01Question 11Not yet answeredMarked out of 15.00Flag questionTipsQuestion textThe electric and magnetic fields of a short dipole (length L << λ) that is placed at the origin and oriented parallel to the z axis of the standard spherical coordinate system can be calculated in the general case at the point r,θ,φ from the following formulaeE⃗ =Erur+Eθuθ𝐸→=𝐸𝑟𝑢𝑟+𝐸𝜃𝑢𝜃 whereEr=j2ωμILcosθe−jkr4πr(1jkr+1(jkr)2)𝐸𝑟=𝑗2𝜔𝜇𝐼𝐿cos⁡𝜃𝑒−𝑗𝑘𝑟4𝜋𝑟(1𝑗𝑘𝑟+1(𝑗𝑘𝑟)2)Eθ=jωμILsinθe−jkr4πr(1+1jkr+1(jkr)2)𝐸𝜃=𝑗𝜔𝜇𝐼𝐿sin⁡𝜃𝑒−𝑗𝑘𝑟4𝜋𝑟(1+1𝑗𝑘𝑟+1(𝑗𝑘𝑟)2) andH⃗ =Hϕuϕ=uϕjkLIsinθe−jkr4πr(1+1jkr)𝐻→=𝐻𝜙𝑢𝜙=𝑢𝜙𝑗𝑘𝐿𝐼sin⁡𝜃𝑒−𝑗𝑘𝑟4𝜋𝑟(1+1𝑗𝑘𝑟)ω is the angular frequency, I is the amplitude of the electric current in the dipole, L is the length of the dipole, and k = 2π/λ is the wave number.(a) Simplify the expression for the wave impedance of a short dipole η=|E⃗ |/|H⃗ |𝜂=|𝐸→|/|𝐻→| as much as possible when θ = 90°. (Keep in mind part b)(b) Using the software of your choice, plot the wave impedance η as a function of the distance-to-wavelength ratio r/λ along the axis perpendicular to the antenna (θ = 90°). Choose, e.g., 0.05≤r/λ≤3 and 0 Ω≤η≤1000 Ω.(c) Mark on the plot i) the level where η = η0 =377 Ω, ii) the distance r/λ = 1/(2π), and iii) the distance r/λ at which η = 0.997η0.(d) What is the reactance of a short dipole like? Which field (E or H) dominates in the distance range r/λ = 1/(2π)? How is this related to the reactance of a short dipole?(e) What distance can be considered as the outer boundary of the reactive near fields of a short dipole?(f) What is the distance of the far field region of a short dipole?(g) How would you assume that the wave impedance curve changes for a small loop antenna? What is the reactance of a small loop, inductive or capacitive?

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