[guided]The simulator should preserve the single-tape computation without encoding or compression. We therefore use tape $1$ of $N$ as the simulated tape of $M$ and make all other tapes irrelevant.
Formally, $N$ has the same state set $Q$ as $M$, so the control state of $N$ directly records the control state of the simulated machine. Its transition function is the map
\begin{align*}
\delta_N: \bigl(Q \setminus \{q_{\mathrm{acc}},q_{\mathrm{rej}}\}\bigr) \times \Gamma^k \to Q \times \Gamma^k \times \{L,R,S\}^k.
\end{align*}
When $N$ is in a nonhalting state $q \in Q \setminus \{q_{\mathrm{acc}},q_{\mathrm{rej}}\}$ and reads symbols $a_1,\dots,a_k \in \Gamma$ on its $k$ tapes, only $a_1$ matters because $a_1$ is the symbol scanned by the simulated single-tape head. If
\begin{align*}
\delta_M(q,a_1) = (q',b,D),
\end{align*}
then $M$ would enter state $q'$, write $b$, and move its head in direction $D$. We define $N$ to do exactly this on tape $1$ and to do nothing on the other tapes:
\begin{align*}
\delta_N(q,a_1,\dots,a_k) = (q',b,a_2,\dots,a_k,D,S,\dots,S).
\end{align*}
This transition is deterministic because $\delta_M$ is deterministic: for each pair $(q,a_1)$ there is exactly one triple $(q',b,D)$, and hence for each tuple $(q,a_1,\dots,a_k)$ there is exactly one transition of $N$. The symbols $a_2,\dots,a_k$ are rewritten unchanged, and the corresponding heads receive the stationary movement $S$, so tapes $2,\dots,k$ remain unused throughout the computation.[/guided]