Dot product in cylindrical coordinates

The dot product of the two vectors in cartesian coordinates is defined as: Multiply corresponding components and the add the results. Thus \( \vec a \cdot \vec b=a_1b_1+a_2b_2+a_3b_3\) If there are two vectors in cylindrical coordinates, \(\vec{A} = A_r \hat{r} + A_\theta \hat{\theta} + A_z \hat{z}\) \(\vec{B} = B_r \hat{r} + B_\theta \hat{\theta} + B_z … Read more

Differential operators in curvilinear coordinates

We have to use the cylindrical coordinates when the problem is cylindrical symmetry. For example, the eigenmode in a circular waveguide. Althrough there is a general theory for the differential operators in general curvilinear coordinates, it it very difficult to be understanded. There is also the formular for the differential operators in cylindrical coordinates. However … Read more

Maxwell’s equation

Maxwell’s equation in vacuum Name Integral equations Differential equations Gauss’s law   Gauss’s law for magnetism Maxwell–Faraday equation(Faraday’s law of induction) Ampère’s circuital law (with Maxwell’s addition) Next, We obtain the electromagnetic wave equation in a vacuum. It is also called Helmholtz equation. Take the Curl of the Faraday equation \(\nabla \times \left(\nabla \times \mathbf {E} \right)=\nabla \times … Read more