$\delta\mathfrak{H}=\delta{g^{ik}R}_{ik}-\frac{1}{2}g^{ik}\delta\left[l,ik+l,ki-2l,s\Gamma_{ik}^s\right]$ | $-g_{\ ,i,k}^{ik}$
Call number 33-171:
(the First Line containing the expression appears twice: once as originally written, with parts of the line struck out, and once ignoring the strikeouts – in addition, the First Line of the second page of the document appears):
$\frac{\partial^2T_{\mu\nu}A^{\mu\nu}}{\partial{x_4}^2}=\frac{T_{\mu\nu\require{cancel}\cancel{\sigma\tau}}A^{\mu\nu}\require{cancel}\cancel{n^\sigma}\left|n\right|}{T_{44}n^4n^4}=\frac{\mathcal{E}_{\mu\nu\sigma\tau}A^{\mu\nu}n^\sigma n^\tau}{T_{\sigma\tau}n^\sigma n^\tau}$
$\frac{\partial^2T_{\mu\nu}A^{\mu\nu}}{\partial{x_4}^2}=\frac{T_{\mu\nu\sigma\tau}A^{\mu\nu}n^\sigma\left|n\right|}{T_{44}n^4n^4}=\frac{\mathcal{E}_{\mu\nu\sigma\tau}A^{\mu\nu}n^\sigma n^\tau}{T_{\sigma\tau}n^\sigma n^\tau}$
$\require{cancel}\cancel{\delta\varphi_{,\mu}=}$ $\require{cancel}\cancel{\delta\varphi=\frac{\partial\varphi}{\partial x_\tau}\delta x_\tau}$
$\delta\varphi_{,\mu}=$ $\delta\varphi=\frac{\partial\varphi}{\partial x_\tau}\delta x_\tau$
