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Multiplying the vertical induction equation by $B$ and averaging eliminates advection and givesIntegrate the derivatives of $A$ by parts. Mixed derivatives of $U$ cancel, leavingThe pointwise cross-product bound and the Cauchy-Schwarz inequality bound its absolute value by $Q\sqrt{⟨A^2⟩⟨|\nabla B{|}^2⟩}$, where $Q=\Vert \nabla U{\Vert }_{\infty }$. HenceFor $J=⟨|\nabla B{|}^2⟩$ and $X=⟨A^2⟩$, completing the square givesApply part (i) and integrate, obtaining the periodic two-coordinate anti-dynamo energy boundThe printed bound has only one power of diffusivity and is false as written. Both powers above are needed: one comes from maximizing against diffusion and the other from integrating the decay time of $A$.

For an explicit counterexample in a nondimensional $2\pi$-periodic box, take $u=(0,0,\sin y)$, $A(x,y,0)=\cos x$, $B(x,y,0)=0$, $k=1$. All means vanish and the velocity is solenoidal. The exact solution isIndeed $B_h\cdot \nabla U=e^{-\eta t}\sin x\cos y$ and this mode's Laplacian is $-2B$. Here $A_0^2=1/2$, $Q=1$, and at $t=(\log 2)/\eta$,For $\eta =0.01$ this is $156.25$, exceeding the printed $1/(8\eta )=12.5$. The corrected bound is valid and finite.