Science, Tensor, Electromagnetic.
things are true for E2 and E3. For B components: We can use the same way for B2 and B3. By defining a tensor Then: iE1 = F41, B1 = F23, and so on. Calculation of all tensor {F} components that have Fμν elements are By this definition, this tensor should be an antisymmetry tensor, because Fμν = -