\begin{align} CNOT |01\rangle &= CNOT \big( |0\rangle \otimes |1\rangle \big) \\
&= \big( |0\rangle \langle 0| \otimes I + |1\rangle \langle 1| \otimes X \big) \big( |0 \rangle \otimes 1\rangle \big) \\
&= \big( |0\rangle \langle 0| \otimes I \big)|0\rangle\otimes|1\rangle + |1\rangle \langle 1| \otimes X \big) |0 \rangle \otimes |1\rangle \\
&= \big(|0\rangle \langle0|\big)|0\rangle \otimes I|1\rangle + \big( |1\rangle \langle 1| \big)|0 \rangle \otimes X|1\rangle\\
&= |0\rangle\otimes|1\rangle + \vec{0} = |01\rangle
\end{align}
So when the controlled qubit is in the state $|0\rangle$, the CNOT gate have no effect on the state.
Qiskit uses little endian so $|01\rangle$ here is essentially the same as your $|10\rangle$ (reading it backward). So the CNOT gate doesn't do anything to the state $|10\rangle$ since the controlled qubit is in the state $|0 \rangle$.
You end with the state $|10\rangle$ in the circuit above at the barrier because your control qubit is in the state $|0\rangle$ and your target qubit is in the state $|1\rangle$ before the CNOT gate. Thus the state stays the same as $|10\rangle$. Also note that the barrier has no physical meaning.