Solving Constants for Prolate Spheroidal Core Wrapped with N Turns of Wire

In summary, to solve the constants for a solid permeable prolate spheroidal core with N turns of wire, using separation of variables and boundary conditions, one must carefully review the equations and do some background research before substituting the boundary conditions, using the orthogonality of the prolate spheroidal functions, and solving for the unknown constants. This may involve multiple iterations and the help of colleagues or a mentor.
  • #1
billybob5588
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Homework Statement



I'm attempting to solve the constants that are attained after using separation of variables for a solid permeable prolate spheroidal core wrapped with N turns of wire using boundary conditions.

H[itex]^{1}_{\delta}[/itex] inside core

H[itex]^{2}_{\delta}[/itex] insulation

H[itex]^{3}_{\delta}[/itex] outside

Homework Equations



H[itex]^{1}_{\delta}[/itex] = K [itex]\Sigma[/itex][itex]^{∞}_{n=1}[/itex] B[itex]_{n}[/itex]P[itex]^{1}_{n}[/itex]([itex]\delta[/itex])P[itex]_{n}[/itex]([itex]\eta[/itex])...(1)

H[itex]^{2}_{\delta}[/itex] = K [itex]\Sigma[/itex][itex]^{∞}_{n=1}[/itex] P[itex]^{1}_{n}[/itex]([itex]\delta[/itex])C[itex]_{n}[/itex][P[itex]_{n}[/itex]([itex]\eta[/itex])+D[itex]_{n}[/itex]Q[itex]_{n}[/itex]([itex]\eta[/itex])]...(2)

H[itex]^{3}_{\delta}[/itex] = K [itex]\Sigma[/itex][itex]^{∞}_{n=1}[/itex] E[itex]_{n}[/itex]P[itex]^{1}_{n}[/itex]([itex]\delta[/itex])Q[itex]_{n}[/itex]([itex]\eta[/itex])...(3)

The conditions are:

H[itex]^{2}_{\delta}[/itex] = H[itex]^{1}_{\delta}[/itex]...(4)

H[itex]^{3}_{\delta}[/itex] - H[itex]^{2}_{\delta}[/itex] = Surface current density...(5)


The Attempt at a Solution



H[itex]^{2}_{\delta}[/itex] = H[itex]^{1}_{\delta}[/itex]

K [itex]\Sigma[/itex][itex]^{∞}_{n=1}[/itex] P[itex]^{1}_{n}[/itex]([itex]\delta[/itex])C[itex]_{n}[/itex][P[itex]_{n}[/itex]([itex]\eta[/itex])+D[itex]_{n}[/itex]Q[itex]_{n}[/itex]([itex]\eta[/itex])] = K [itex]\Sigma[/itex][itex]^{∞}_{n=1}[/itex] B[itex]_{n}[/itex]P[itex]^{1}_{n}[/itex]([itex]\delta[/itex])P[itex]_{n}[/itex]([itex]\eta[/itex])...(6)

K [itex]\Sigma[/itex][itex]^{∞}_{n=1}[/itex] cancel out also P[itex]^{1}_{n}[/itex]([itex]\delta[/itex]) are orthogonal and cancel out. Therefore left with;

C[itex]_{n}[/itex][P[itex]_{n}[/itex]([itex]\eta[/itex])+D[itex]_{n}[/itex]Q[itex]_{n}[/itex]([itex]\eta[/itex])] = B[itex]_{n}[/itex]P[itex]_{n}[/itex]([itex]\eta[/itex])

Solve for B[itex]_{n}[/itex] C[itex]_{n}[/itex] or D[itex]_{n}[/itex]?

Where do I go from here? If i sub this back into (6) doesn't get me anywhere. Unless I am missing something obvious.

Thanks,
 
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  • #2


your first step would be to carefully review the equations and boundary conditions given and make sure that they are correct. You can also do some background research on prolate spheroidal coordinates and the use of separation of variables in solving this type of problem.

Once you have a solid understanding of the problem and its mathematical formulation, you can start by substituting the boundary conditions (4) and (5) into the equations (1), (2), and (3). This will help you eliminate some of the unknown constants and simplify the equations.

Next, you can use the orthogonality of the prolate spheroidal functions to solve for the remaining unknown constants. This may involve some algebraic manipulation and possibly using some known identities for the prolate spheroidal functions.

Once you have solved for all the constants, you can then substitute them back into the original equations (1), (2), and (3) to obtain the final solution for H^{1}_{\delta}, H^{2}_{\delta}, and H^{3}_{\delta}.

It's important to keep in mind that solving this type of problem can be complex and may require multiple iterations and careful checking of the solution. It's also helpful to consult with colleagues or a mentor for guidance and to double-check your work. Good luck!
 

Related to Solving Constants for Prolate Spheroidal Core Wrapped with N Turns of Wire

1. What is a prolate spheroidal core?

A prolate spheroidal core is a three-dimensional shape that resembles an elongated sphere. It is used in many scientific applications, including as a basis for solving constants for prolate spheroidal cores wrapped with wire.

2. Why is it important to solve constants for prolate spheroidal cores?

Solving constants for prolate spheroidal cores allows for accurate calculations and predictions in various scientific and engineering fields. This information can be used to design and optimize devices such as antennas, sensors, and medical equipment.

3. How is the number of turns of wire determined in this problem?

The number of turns of wire is determined by the desired properties and performance of the core. It must be optimized to achieve the desired magnetic field and other characteristics. This number can be calculated using equations and formulas based on the specific properties of the core and wire.

4. What factors affect the constants for a prolate spheroidal core?

The constants for a prolate spheroidal core are affected by various factors, including the material and dimensions of the core, the number of turns of wire, and the frequency of the electrical signal. These factors can impact the magnetic field, inductance, and other properties of the core.

5. How can the constants for a prolate spheroidal core be solved?

The constants for a prolate spheroidal core can be solved using mathematical methods and techniques, such as numerical analysis and optimization algorithms. These methods involve solving equations and finding the optimal values for the constants based on the given parameters and constraints.

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