The text I am reading has the following
$$E=(I+\nabla I\frac{\partial W}{\partial p}\Delta p -T)^2$$ where $\nabla I$ us a row vector $1$ by $2$, $\frac{\partial W}{\partial p}$ is a $2$ by $3$ matrix and $\Delta p$ is a $3$ by $1$ column vector. $I$ and $T$ are scalars. We seek the gradient $\frac{\partial E}{\partial \Delta p_k}$, but I do not understand their solution. I will present my attempt, and than their solution.
In index notation, we have $(I+\nabla I_i\frac{\partial W^i}{\partial \Delta p_k}\Delta p^k -T)^2$, where summation if implied by repeated indicies, Than the derivative is
$$\frac{\partial E}{\partial \Delta p_m}=2(I+\nabla I_i\frac{\partial W^i}{\partial p_k}\Delta p^k -T)\nabla I_n\frac{\partial W^n}{\partial p_m}$$ or returning to the matrix notation
$$\frac{\partial E}{\partial \Delta p}=2(I+\nabla I\frac{\partial W}{\partial p}\Delta p -T)\nabla I\frac{\partial W}{\partial p}\tag{1}\label{1}$$
But their solution is
$$\frac{\partial E}{\partial \Delta p}=2(\nabla I\frac{\partial W}{\partial p})^T(I+\nabla I\frac{\partial W}{\partial p}\Delta p -T)\tag{2}\label{2}$$
Why is their solution correct and where did I make the mistake? My solution is equation \eqref{1}, but theirs is \eqref{2}. I am confused, why in theirs, $$(\nabla I\frac{\partial W}{\partial p})$$ is transposed?
It looks like the text you are reading uses so-called Denominator layout, for matrix calculus notation, i.e. given two column vectors $\boldsymbol{x}\in\mathbb{R}^m$ and $\boldsymbol{y}\in\mathbb{R}^n$ of the size $m\times1$ and $n\times1$ respectively we write derivative $\displaystyle\dfrac{\partial \boldsymbol{y}}{\partial\boldsymbol{x}}$ as $n\times m$ matrix. In other words, the layout is according to $\boldsymbol y^{\boldsymbol\top}$ and $\mathbf{x}$.
In your case $E$ is the scalar, so that $n=1$ and $m=3$, and thus the derivative of scalar w.r.t. the vector $\Delta p$ has to be a column vector of the size $3\times1$.
More details are available, for example, on the Wikipedia page for Matrix Calculus.
Moreover, using provided there table of scalar-by-vector identities one can figure out dimensionality of each term emerging from the chain rule explicitly. According to the linked table,
Using this identity, you can easily see that $$ \frac{\partial }{\partial \Delta p} \left( \nabla I\frac{\partial W}{\partial p}\Delta p\right) = \left( \nabla I\frac{\partial W}{\partial p}\right)^{\boldsymbol\top} $$