A two-dimensional oblique lattice has basis vectors and (Cartesian components in an…

PHYSICS · Multi-part · Fermi University Physics · Mathematical Methods for Physics · Tensors and differential geometry · Tensors and differential geometry

Invariance, Ch General bases, the metric and tensors in spacetime

Problem

A two-dimensional oblique lattice has basis vectors e1=(2,0) m\mathbf{e}_1 = (2, 0)\,\mathrm{m} and e2=(1,3) m\mathbf{e}_2 = (1, 3)\,\mathrm{m} (Cartesian components in an auxiliary orthonormal frame). A vector has contravariant components Vi=(3,1)V^i = (3, 1) in this basis. Someone argues: "To lower the index I just write Vi=δijVjV_i = \delta_{ij}V^j, so V1=3V_1 = 3 and V2=1V_2 = 1: lowering an index never changes the numbers, it only changes where you write them." ((a)) Explain what is wrong with this reasoning. ((b)) Compute the correct covariant components ViV_i. ((c)) Use ViViV^iV_i to find the length ∣V∣|\mathbf{V}|, and check it is not 32+12 m=10 m\sqrt{3^2+1^2}\,\mathrm{m} = \sqrt{10}\,\mathrm{m}.

Browse the problem library