I am studying geometric measure theory ([Herbert Federer - Geometric measure theory](https://link.springer.com/book/10.1007/978-3-642-62010-2)) and I have a question about class $r$ homotopies. Here's the definition, from p. 363, Section 4.1.9:
> Suppose $U$ is an open subset of $\mathbb{R}^{n}$, $V$ is an open subset of $\mathbb{R}^{v}$ $f$, and $g$ are functions mapping $U$ into $V$. A homotopy of class $r$ from $f$ to $g$ is a map
$$
h: A \times U \rightarrow V
$$
of class $r$ such that $A$ is an open subinterval of $\mathbb{R}$, $0 \in A$, $1 \in A$,
$$
h(0, x)=f(x) \text { and } h(1, x)=g(x) \text { for } x \in U.
$$
Whenever $t \in A$ we define
$$
h_{t}: U \rightarrow V, \quad h_{t}(x)=h(t, x) \text { for } x \in U,
$$
hence $h_{0}=f$ and $h_{1}=g$; in case $r \geq 1$ we also define
$$
h_{t}: U \rightarrow \mathbb{R}^{v}, \quad h_{t}(x)=\langle(1,0), D h(t, x)\rangle \text { for } x \in U,
$$
hence $\langle(v, w), D h(t, x)\rangle=v h_{t}(x)+\left\langle w, D h_{t}(x)\right\rangle$ for $t \in A$, $x \in U$, $v \in \mathbb{R}$, $w \in \mathbb{R}^{n}$.

Now my question is about the last 3 lines: 
> in case $r \geq 1$ we also define
$$
h_{t}: U \rightarrow \mathbb{R}^{v}, \quad h_{t}(x)=\langle(1,0), D h(t, x)\rangle \text { for } x \in U,
$$
hence $\langle(v, w), D h(t, x)\rangle=v h_{t}(x)+\left\langle w, D h_{t}(x)\right\rangle$ for $t \in A, x \in U, v \in \mathbb{R}, w \in \mathbb{R}^{n}$.

Actually, we know that $\langle v, Df(a)\rangle = v \cdot \nabla f(a)$. Also, in the last line it is mentioned that $w \in \mathbb{R}^n$, hence $0 = (0, \dotsc,0) \in \mathbb{R}^n$. Now, we have:
$$h_t(x)= \langle (1, 0, \dotsc, 0), Dh(t,x) \rangle$$ which is equal to 
\begin{align} h_t(x) &= (1, 0, \dotsc, 0) \cdot \nabla h(t,x)\\ &= (1, 0 , \dotsc, 0) \cdot \left(\frac{\partial h}{\partial t}, \frac{\partial h}{\partial x_1}, \dotsc, \frac{\partial h}{\partial x_n}\right) \\
&= \frac{\partial h}{\partial t}.\end{align}

Now, my question is that why it is said that $h_t: U \rightarrow \mathbb{R}^{\nu}$? I mean, now we should see that $\frac{\partial h}{\partial t} \in \mathbb{R}^{\nu}$, but I don't get it really! If this is just the differential of $h$, it must lie in $\mathbb{R}^{n-1}$!