Green's reciprocity theorem about current density and magnetic field

In summary: Since all three terms are equal to zero, the equation is true.In summary, the conversation is discussing the proof of three equations related to electric and magnetic fields. The first two equations can be proven using a definition of the electric field, however, the third equation cannot be proven using a definition of the magnetic field. It is suggested that all three equations are related to Newton's third law of Lorentz force and someone may know how to prove them. The third equation can be proved by expanding the cross products and showing that all three terms are equal to zero.
  • #1
SanaiBongchul
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2
Homework Statement
I have to prove the Green's reciprocity theorem about the Electric field, electric potential, and magnetic field.
Relevant Equations
Intgral over all space J_2 cross B_1 = -Integral over all space J_1 cross B_2
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I have to prove three equations above.
For first two equations, I've been thought and made reasonable answer by using a definition of the electricfield.
However, for third, I can't use a definition of a magnetic field due to the cross product
Like J_2 X J_1 X (r_2 - r_1).
I think three of 'em are kinda related to Newton's third law of lorentz force.
Does anyone know about the proof?
Or would you think you can prove these?
 
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  • #2
A:The third equation is simply a vector identity, and can be proved by expanding the cross products. $$\mathbf{J}_2 \times \mathbf{J}_1 \times (\mathbf{r}_2 - \mathbf{r}_1) = (\mathbf{r}_2 - \mathbf{r}_1)\cdot(\mathbf{J}_2 \times \mathbf{J}_1) - (\mathbf{J}_2 \cdot (\mathbf{r}_2 - \mathbf{r}_1))\mathbf{J}_1 + (\mathbf{J}_1 \cdot (\mathbf{r}_2 - \mathbf{r}_1)) \mathbf{J}_2$$The left-hand side of the equation is clearly zero, so the two terms on the right-hand side must also be equal to zero. The first term is equal to zero because the dot product of two vectors perpendicular to each other is zero. The second and third terms are equal to zero because $\mathbf{J}_2$ and $\mathbf{J}_1$ are constant, so they cannot depend on $\mathbf{r}_2 - \mathbf{r}_1$.
 

FAQ: Green's reciprocity theorem about current density and magnetic field

What is Green's reciprocity theorem about current density and magnetic field?

Green's reciprocity theorem states that the current density at a point in a magnetic field is equal to the magnetic field at that point due to a unit current density source at another point. In other words, the relationship between current density and magnetic field is reciprocal.

How is Green's reciprocity theorem used in practical applications?

Green's reciprocity theorem is often used in the design and analysis of electromagnetic devices, such as motors, generators, and transformers. It helps engineers and scientists understand the relationship between current density and magnetic field and how changes in one can affect the other.

Can Green's reciprocity theorem be applied to all types of magnetic fields?

Yes, Green's reciprocity theorem can be applied to all types of magnetic fields, including static, steady-state, and time-varying fields. It is a fundamental principle in electromagnetism and is applicable in a wide range of scenarios.

What is the mathematical expression for Green's reciprocity theorem?

The mathematical expression for Green's reciprocity theorem is J(x) = B(y), where J(x) is the current density at point x and B(y) is the magnetic field at point y due to a unit current density source at point x.

Are there any limitations to Green's reciprocity theorem?

Green's reciprocity theorem is based on the assumptions of linearity and isotropy, which may not always hold true in practical situations. Additionally, it only applies to steady-state or time-harmonic fields, and may not be valid for transient fields. Therefore, it is important to carefully consider the limitations and applicability of Green's reciprocity theorem in any given scenario.

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