Step 1: In the Einthoven triangle, the axis of Lead II is at \(+60^\circ\) with respect to the horizontal (Lead I at \(0^\circ\)). The measured lead voltage equals the projection of the dipole vector on the lead axis:
\[
V_{\text{lead}} = M \cos(\theta_{\text{dipole}}-\theta_{\text{lead}}).
\]
Step 2: Here \(M=3\) mV, \(\theta_{\text{dipole}}=-45^\circ\), \(\theta_{\text{lead}}=60^\circ\). Hence
\[
|V_{II}| = 3\,|\cos(60^\circ-(-45^\circ))| = 3\,|\cos(105^\circ)|
= 3\times 0.2588 \approx 0.78\ \text{mV}.
\]
Therefore, the magnitude of the Lead II signal is \(\boxed{0.78\ \text{mV}}\).