= Solution
In coordinates $x^\mu$, write the type-$(1,1)$ tensor as
$$
T=T^\mu{}_{\nu}\,
\partial_\mu\otimes dx^\nu.
$$
For a covector $\eta=\eta_\mu dx^\mu$ and vector $V=V^\nu\partial_\nu$,
$$
T(\eta,V)=T^\mu{}_{\nu}\eta_\mu V^\nu.
$$
Since this must equal $\eta(V)=\eta_\nu V^\nu$ for every $\eta$ and $V$, the components are
$$
\boxed{T^\mu{}_{\nu}=\delta^\mu{}_{\nu}}.
$$
Thus $T$ is the <identity tensor>.
The <tensor component transformation law> gives
$$
\begin{aligned}
T^{\mu'}{}_{\nu'}
&=\frac{\partial x^{\mu'}}{\partial x^\alpha}
\frac{\partial x^\beta}{\partial x^{\nu'}}
T^\alpha{}_{\beta}\\
&=\frac{\partial x^{\mu'}}{\partial x^\alpha}
\frac{\partial x^\alpha}{\partial x^{\nu'}}\\
&=\delta^{\mu'}{}_{\nu'}.
\end{aligned}
$$
The components are therefore the same <Kronecker delta> in every coordinate system.
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