Proving that J[transverse] + J[longitudinal] = J, where J = current density

In summary, as a scientist, it is important to question and evaluate methods and assumptions. While using the equation in question may seem like the only way to get a Dirac delta to appear later, alternative methods should also be considered and the validity of the approach should be checked. Consulting with colleagues or experts in the field can also help validate the approach and ensure it aligns with accepted practices. Ultimately, as long as the solution is logically and mathematically sound, it may not necessarily be "wrong" to use the equation, but critical evaluation and adherence to accepted practices is important.
  • #1
bjnartowt
284
3

Homework Statement



see attached .pdf

Homework Equations



see attached .pdf

The Attempt at a Solution



see attached .pdf

Question: am I wrong for using,
[tex]{{\bf{J}}_\ell } \equiv - \frac{1}{{4\pi }}\nabla \int {\frac{{\nabla ' \bullet {\bf{J}}({\bf{x'}})}}{{\left| {{\bf{x}} - {\bf{x'}}} \right|}}{d^3}x'} = - \frac{1}{{4\pi }}\nabla \left( {\nabla \bullet \int {\frac{{{\bf{J}}({\bf{x'}})}}{{\left| {{\bf{x}} - {\bf{x'}}} \right|}}{d^3}x'} } \right)[/tex]

in Eq. [I.4] of the attached .pdf? It seems the only way to get a Dirac delta to appear later, which I need...
 

Attachments

  • 294 - pr 26 - transverse and longitudinal decomposition.pdf
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  • #2


it is important to always question and evaluate your methods and assumptions. While it may seem like using this equation is the only way to get a Dirac delta to appear later, it is important to consider alternative methods and approaches as well. It is also important to check your calculations and make sure that your use of this equation is valid and consistent with the principles of the field. Consulting with colleagues or seeking guidance from experts in the field can also help to validate your approach and ensure that you are on the right track. Ultimately, as long as your solution is logically and mathematically sound, it is not necessarily "wrong" to use this equation. However, it is always important to critically evaluate your methods and make sure they align with accepted practices in the field.
 

Related to Proving that J[transverse] + J[longitudinal] = J, where J = current density

1. What is the significance of proving J[transverse] + J[longitudinal] = J?

The equation J[transverse] + J[longitudinal] = J is significant because it represents the conservation of electric current. This means that the total current flow in a system remains constant, even when it is divided into transverse and longitudinal components.

2. How is current density (J) defined?

Current density (J) is defined as the amount of electric current flowing through a unit area per unit time. It is represented by a vector quantity, with both magnitude and direction.

3. How can this equation be proven?

This equation can be proven using vector calculus and the principles of electromagnetism. It involves breaking down the current density into its transverse and longitudinal components, and then manipulating the equations to show that the sum of these components is equal to the total current density.

4. What are some real-world applications of this equation?

This equation has many applications in electrical engineering and physics. It is used in the design of electrical circuits, the study of electromagnetic waves, and the analysis of current flow in materials such as semiconductors and superconductors.

5. Are there any exceptions to this equation?

While this equation holds true in most cases, there are some situations where it may not apply. For example, in the presence of strong magnetic fields or when dealing with non-linear materials, the equation may need to be modified to account for these factors.

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