The answer is that if we consider the particularization of the $n$-dimensional BV norm for $n=1$, i.e.
$$\DeclareMathOperator{\Dm}{d\!}
\Vert f\Vert_{BV} \triangleq \Vert f\Vert_{L_1}+\operatorname{TV}(f)\label{1}\tag{1}
$$ where
$\operatorname{TV}(f)$ is the Tonelli-Cesari total variation as given in the OP and in my comment, the operator $T(f)$ is discontinuous.
On the other hand, if we consider the classical $1$-dimensional BV norm
$$
\Vert f\Vert_\mathscr{BV} \triangleq \Vert f\Vert_{L_1}+\operatorname{\mathscr{V}}(f)\label{2}\tag{2}
$$
where
$$
\operatorname{\mathscr{V}}(f)=\sup_{P \in \mathscr{P}} \sum_{i=0}^{n_{P}-1} | f(x_{i+1})-f(x_i) |
$$
is the classical (or we may say Jordan) variation of $f$ and $\mathscr{P}$ is the set of finite partitions of $\Bbb R$, then $T(f)$ is continuous.
Proof of the discontinuity of $T(f)$ respect to $\Vert \cdot\Vert_{BV}$. Consider $f$ as the characteristic function of the open interval $]0, 1[$, i.e.
$$
f(x) \triangleq\chi_{]0,1[}(x)=
\begin{cases}
1 & x\in ]0,1[,\\
0 & x\notin ]0,1[.
\end{cases}
$$
As we can easily prove, $f\in BV(\Bbb R, [0,1])$: now let's define a sequence $\{f_n\}_{n\in\Bbb N_{>0}}\subsetneq BV(\Bbb R, [0,1])$ converging to $f$ as
$$
f_n(x)\triangleq
\begin{cases}
\varphi_n\ast f(x) = \displaystyle\int\limits_{\Bbb R}\varphi_n(x-y)f(y)\Dm y = \int\limits_0^1\varphi_n(x-y)\Dm y &x\neq 0,\\
1-\frac{1}{2}\sin\frac{1}{n} & x=0.
\end{cases}
$$ where $\varphi_n(x)$ is any sequence of $C^\infty_0$ mollifiers converging to the Dirac measure as $n\to\infty$: note that also $f_n(x)\to f(x)$ pointwise for all $x\in\Bbb R\setminus\{0\}$, while for $x=0$ the pointwise limit does not exist due to the rapid oscillations of the function sequence at that point.
Now it's easy to see that
$$
\Dm f = \delta(0)-\delta(1) = \lim_{n\to\infty} \Dm f_n\;\text{ in the space of Radon measures }\;\mathcal{M}(\Bbb R).\label{3}\tag{3}
$$
and while this implies that
$$
\int (h\circ f) \Dm f = h\circ f(0) - h\circ f(1) =h(0)-h(0)=0
$$
it also implies that $T(f_n)\nrightarrow 0$ as $n\to\infty$ since for a sufficiently large $n$ we have that
$$
\begin{split}
T(f_n) &= \int (h\circ f_n) \Dm f_n = \int\limits_{\Bbb R} (h\circ f_n) \Dm f_n \\
& = \int\limits_{\Bbb R} (h\circ f_n) \Dm f_n + h \circ f_n(0) - h \circ f_n(1) - h \circ f_n(0) + h \circ f_n(1)\\
& = h \circ f_n(0) - h \circ f_n(1) \\
& \qquad\qquad+ \int\limits_{-\infty}^{+\frac 12} \big(h\circ f_n- h \circ f_n|_{x=0}\big) \Dm f_n + \int\limits_{1\over 2}^{+\infty} \big(h \circ f_n - h\circ f_n|_{x=1}\big) \Dm f_n\\
& = h \left(1-\frac{1}{2}\sin\frac{1}{n} \right) - h \circ f_n(1)\\
& \qquad\qquad + \int\limits_{-\infty}^{+\frac 12} \big(h\circ f_n- h \circ f_n|_{x=0}\big) \Dm f_n + \int\limits_{1\over 2}^{+\infty} \big(h \circ f_n - h\circ f_n|_{x=1}\big) \Dm f_n
\end{split}\label{4}\tag{4}
$$
Now while the last three terms on the right side converge to a limit for $n\to\infty$, precisely
$$
\begin{align}
\lim_{n\to\infty} & h \circ f_n(1) = h(0), \\
\lim_{n\to\infty} & \int\limits_{-\infty}^{+\frac 12} \big(h\circ f_n- h \circ f_n|_{x=0}\big) \Dm f_n = 0, \\
\lim_{n\to\infty} & \int\limits_{1\over 2}^{+\infty} \big(h \circ f_n - h\circ f_n|_{x=1} \big) \Dm f_n = 0
\end{align}
$$
the first term, i.e. $h \left(1-\frac{1}{2}\sin\frac{1}{n} \right)$ does not, thus $\vert T(f_n) - T(f)\vert \nrightarrow 0$ for $n\to\infty$ and the functional $T:{BV}(\Bbb R, [0,1]) \to \Bbb R$ is not continuous respect to the topology of ${BV}(\Bbb R, [0,1])$.
Proof of the continuity of $T(f)$ respect to $\Vert \cdot \Vert_\mathscr{BV}$. This is simply a consequence of the fact that $\Vert \cdot \Vert_\mathscr{BV}$ forces any converging sequence in the corresponding Banach space $\mathscr{BV}(\Bbb R, [0,1])$ to converge also pointwisely.
Final notes.
- In the development above, for the sake of clarity I've adopted some non standard notations: precisely in the literature $\mathscr{V}(f)$ is $V(f)$ and we speak of BV spaces with norm $\|\cdot\|_{BV}$ defined by \eqref{1} or \eqref{2}, leaving to the analysis of the context the understanding of what of the two is effectively used.
- The problem (as in this Q&A) is exactly the one also pointed out by Liding Yao in his comment: $
\{f_n\}_{n\in\Bbb N_{>0}}$ should be pointwise known on the support of the singular part of the Radon measure defined by its limit $f$, and this cannot be guaranteed if you are working in BV.
- Perhaps a clearer explanation of the passages of why relations \eqref{3} and \eqref{4} hold is needed. These equations are consequences of the fact that $\{\varphi_n\}_{n\in}\subsetneq C_o^\infty(\Bbb R)$ is a sequence of smooth mollifiers.