The actual angle of dip \( \delta \) can be determined using the relationship between the angle of suspension \( \theta \), the magnetic declination (the angle with the magnetic meridian), and the angle of dip. The formula to calculate the actual angle of dip is given by:
\[
\tan(\delta) = \tan(\theta) \times \cos(\alpha)
\]
where:
- \( \delta \) is the actual angle of dip,
- \( \theta = 45^\circ \) is the angle between the magnet and the horizontal,
- \( \alpha = 30^\circ \) is the angle the magnet makes with the magnetic meridian.
Substituting the values into the equation:
\[
\tan(\delta) = \tan(45^\circ) \times \cos(30^\circ)
\]
We know that \( \tan(45^\circ) = 1 \) and \( \cos(30^\circ) = \frac{\sqrt{3}}{2} \). Therefore:
\[
\tan(\delta) = 1 \times \frac{\sqrt{3}}{2} = \frac{\sqrt{3}}{2}
\]
Now, to find \( \delta \), we take the inverse tangent of both sides:
\[
\delta = \tan^{-1}\left( \frac{\sqrt{3}}{2} \right)
\]
Using a calculator:
\[
\delta \approx 60^\circ
\]
Thus, the actual angle of dip is approximately:
\[
\boxed{60^\circ}
\]