Our presentation is therefore organized in such a way that the analogies between the concepts of topological space and continuous function, on the one hand, and of measurable space and measurable function, on the other, are strongly emphasized.
On the other hand, $F$ fails to have property $P$. [Not: “On the other side”]
With Lemma 4 in $\langle$at$\rangle$ hand, we can finally define $E$ to be equal to $P(m)/H$.
Once the dissipation relation is in hand, no further work is required.
It can be easily calculated by hand that the nonzero solutions are ......
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