Inviscid Limit for Yudovich solution to heat conductive Boussinesq equation on two-dimensional periodic domain

We establish the inviscid limit of the Yudovich solution to the heat conductive Boussinesq equation with initial velocity and temperature/buoyancy in $L^2$ and initial vorticity in $L^{\mathrm{\infty }}$ on the two-dimensional periodic domain ${\mathbf{T}}^2$. Given any finite time $T>0$ and $p\in [1,\mathrm{\infty }[$, we show that the solution to the diffusive Boussinesq equation converges in $L^{\mathrm{\infty }}(0,T;W^{1,p}({\mathbf{T}}^2))$ to the solution to the Euler–Boussinesq equation as the viscosity tends to zero, provided that the initial vorticity, velocity, and temperature/buoyancy converge strongly in $L^2$. Our proof adapts and extends the arguments in [P. Constantin, T. D. Drivas, and T. M. Elgindi, Comm. Pure Appl. Math. 75 (2022), 60–82] to forcing terms in $L^1(0,T;L^{\mathrm{\infty }}({\mathbf{T}}^2))$.