Let $f:\mathbb{R}^{m+n}\to \mathbb{R}^m,\ \mathbf{t}=[x_1,\cdots,x_m,y_1,\cdots,y_n]\to [f_1(\mathbf{t}),\cdots,f_m(\mathbf{t})]$ be a differentiable function. Here $[a_1,\cdots,a_m]$ means a column vector with a height of $m.$ I think that the symbol $\partial f\over {\partial \mathbf{y}}$ represents the matrix \begin{equation*} \left( \begin{array}{cccc} \displaystyle{{\partial f_1}\over {\partial y_1}}&\displaystyle{{\partial f_1}\over {\partial y_2}}&\cdots&\displaystyle{{\partial f_1}\over {\partial y_n}}\\ \displaystyle{{\partial f_2}\over {\partial y_1}}&\displaystyle{{\partial f_2}\over {\partial y_2}}&\cdots&\displaystyle{{\partial f_2}\over {\partial y_n}}\\ \vdots&\vdots&\ddots&\vdots\\ \displaystyle {{\partial f_m}\over {\partial y_1}}&\displaystyle{{\partial f_m}\over {\partial y_2}}&\cdots&\displaystyle{{\partial f_m}\over {\partial y_n}} \end{array} \right) , \end{equation*} so when $m=1,$ we have ${\partial f\over {\partial \mathbf{y}}}=({\partial f\over {\partial y_1}},\cdots,{\partial f\over {\partial y_n}}).$ Thus $\partial f\over{\partial\mathbf{y}}$ is a row vector.
But in mechanics the following equation can be seen everywhere: $$m{d\mathbf{v}\over{dt}}=-{\partial U\over \partial{\mathbf{r}}}. $$ But if we view radius vector $\mathbf{r}$ as a column vector, then $\displaystyle{d\mathbf{v}\over{dt}}$ is a column vector, so it seems that $$ {\partial U\over \partial{\mathbf{r}}}=[{\partial U\over {\partial x}},{\partial U\over {\partial y}},{\partial U\over {\partial z}}],$$ which contradicts my definition.
Question: Should the equation be rewritten as $$m{d\mathbf{v}\over{dt}}=-\Big({\partial U\over \partial{\mathbf{r}}}\Big)^T ?$$