Tensor symmetry is an invariant property. The proof shows that if a tensor is symmetric in one coordinate system ( Tab=Tba ), it will always be symmetric in any other transformed coordinate system ( T′a′b′=T′a′b′ ). This is demonstrated by applying the tensor transformation rule and using the initial symmetry to rearrange terms. The fact that the property holds true across all coordinate systems makes symmetry a fundamental characteristic of the tensor itself, rather than a coincidental feature of a specific coordinate representation.