Note that usually, the state $|0+\rangle$ can denote apply the operator $(I \otimes H)$ to the state $|00\rangle$. Hence, it would be the circuit:
$\hspace{8cm}$ Figure 1:
$\hspace{6.5 cm}$ 
and also in a standard textbook, this can be written as $I \otimes H$.
But because qiskit uses little-endian convention, the state $|0+\rangle$ actually actually means the first qubit is $|+\rangle$ and the second qubit is $|0\rangle$. That is, it is in reverse order. Thus, the circuit representation for this state is actually:
$\hspace{8cm}$Figure 2:
$\hspace{7 cm}$
In term of tensor notation, this (gate operation in Figure 2) can be written as $(I \otimes H) |00\rangle$. That is, we read from bottom up instead of top to bottom like what we would have done in standard setting. That is because we reversed the qubit ordering so by doing this we make sure that the gate operation written in tensor notation stay the same as what we would have in standard textbook setting.
And now applying CNOT gate to this circuit we get:
$\hspace{8cm}$Figure 3:
$\hspace{6cm}$ 
In term of the math, first note that usually the matrix representation for CNOT is:
$$CNOT = \begin{pmatrix} 1 & 0 & 0 & 0 \\ 0 & 1 & 0 & 0 \\ 0 & 0 & 0 & 1\\ 0 & 0 & 1 & 0\end{pmatrix} $$
but with little-endian, its matrix representation is
$$CNOT_{little \ endian} = \begin{pmatrix} 1 & 0 & 0 & 0 \\ 0 & 0 & 0 & 1 \\ 0 & 0 & 1 & 0\\ 0 & 1 & 0 & 0\end{pmatrix} $$
and so overall, we applying the operation $U = CNOT_{little \ endian} \cdot (I \otimes H)$ to the state $|00\rangle$. So if we use matrix notation to work this out, we will have the following:
$$
CNOT_{little \ endian} \cdot (I \otimes H) = \begin{pmatrix} 1 & 0 & 0 & 0 \\ 0 & 0 & 0 & 1 \\ 0 & 0 & 1 & 0\\ 0 & 1 & 0 & 0\end{pmatrix} \cdot \dfrac{1}{\sqrt{2}} \begin{pmatrix} 1 & 1 & 0 & 0 \\ 1 & -1 & 0 & 0 \\ 0 & 0 & 1 & 1\\ 0 & 0 & 1 & -1\end{pmatrix} = \dfrac{1}{\sqrt{2}} \begin{pmatrix} 1 & 1 & 0 & 0 \\ 0 & 0 & 1 & -1 \\ 0 & 0 & 1 & 1\\ 1 & 1 & 0 & 0\end{pmatrix}
$$
and now the state $|00\rangle = \begin{pmatrix} 1 \\ 0 \\ 0 \\ 0 \end{pmatrix} $ so therefore $CNOT_{little \ endian} \cdot (I \otimes H) |00\rangle$ can be worked out as:
$$
\big( CNOT_{little \ endian} \cdot (I \otimes H) \big) |00\rangle = \dfrac{1}{\sqrt{2}} \begin{pmatrix} 1 & 1 & 0 & 0 \\ 0 & 0 & 1 & -1 \\ 0 & 0 & 1 & 1\\ 1 & 1 & 0 & 0\end{pmatrix} \begin{pmatrix} 1 \\ 0 \\ 0 \\ 0 \end{pmatrix} = \dfrac{1}{\sqrt{2}} \begin{pmatrix} 1 \\ 0 \\ 0 \\ 1 \end{pmatrix} = \dfrac{|00\rangle + |11\rangle}{\sqrt{2}}
$$