How is the Maxwell stress tensor expressed solely in terms of the magnetic field tensor by using the

How is the Maxwell stress tensor expressed solely in terms of the magnetic field tensor by using the results from parts (a) and (b)?

Take the standard expression for the magnetic Maxwell stress tensor Tik\mathbf{T}{ik} (in terms of B\mathbf{B}) and convert it entirely into an expression involving the magnetic field tensor Fij\mathbf{F}{ij}.

The process involves two main substitutions, using the identity derived in part (b) and the trace of that identity.

📐 Expressing Tik\mathbf{T}{ik} in Terms of Fij\mathbf{F}{ij}

1. Start with the Definition of the Maxwell Stress Tensor

The magnetic part of the Maxwell stress tensor is:

Tik=1μ0(BiBk12B2δik) \mathbf{T}_{ik} = \frac{1}{\mu_0} \left( \mathbf{B}_i \mathbf{B}k - \frac{1}{2} \mathbf{B}^2 \delta{ik} \right)

2. Use the Result from Part (b)

The result derived in part (b) is:

FijFjk=B2δikBiBk \mathbf{F}{ij} \mathbf{F}{jk} = \mathbf{B}^2 \delta_{ik} - \mathbf{B}_i \mathbf{B}_k

Solving this for the dyadic term BiBk\mathbf{B}_i \mathbf{B}_k:

BiBk=B2δikFijFjk \mathbf{B}i \mathbf{B}k = \mathbf{B}^2 \delta{ik} - \mathbf{F}{ij} \mathbf{F}_{jk}

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