In Electromagnetic Field Theory (EMFT), coordinate systems help us describe vectors and fields in space efficiently. Choosing the right coordinate system simplifies both understanding and calculations.
This chapter is extremely important for GATE because most derivations (gradient, divergence, curl) depend on coordinate systems.
Keywords: coordinate systems EMFT, Cartesian cylindrical spherical, coordinate transformation, scale factors EMFT, GATE ECE vectors
Most basic and intuitive coordinate system using x, y, z axes.
$$ \vec{A} = A_x \hat{i} + A_y \hat{j} + A_z \hat{k} $$
Used when symmetry exists around an axis.
Coordinates: $(\rho, \phi, z)$
$$ \vec{A} = A_\rho \hat{\rho} + A_\phi \hat{\phi} + A_z \hat{z} $$
Used when symmetry exists in all directions (point-based).
Coordinates: $(r, \theta, \phi)$
$$ \vec{A} = A_r \hat{r} + A_\theta \hat{\theta} + A_\phi \hat{\phi} $$
$$ x = \rho \cos\phi, \quad y = \rho \sin\phi $$
$$ \rho = \sqrt{x^2 + y^2}, \quad \phi = \tan^{-1}(y/x) $$
$$ x = r \sin\theta \cos\phi $$
$$ y = r \sin\theta \sin\phi $$
$$ z = r \cos\theta $$
$$ r = \sqrt{x^2 + y^2 + z^2} $$
| System | h1 | h2 | h3 |
|---|---|---|---|
| Cartesian | 1 | 1 | 1 |
| Cylindrical | 1 | $\rho$ | 1 |
| Spherical | 1 | $r$ | $r\sin\theta$ |
Why important?
| Feature | Cartesian | Cylindrical | Spherical |
|---|---|---|---|
| Coordinates | (x, y, z) | (ρ, φ, z) | (r, θ, φ) |
| Best For | Rectangular | Wires | Point Charges |
| Complexity | Low | Medium | High |
$$ \vec{A} = A_x \hat{i} + A_y \hat{j} + A_z \hat{k} $$
$$ \vec{A} = A_\rho \hat{\rho} + A_\phi \hat{\phi} + A_z \hat{z} $$
$$ \vec{A} = A_r \hat{r} + A_\theta \hat{\theta} + A_\phi \hat{\phi} $$
Discussion / Comments