Step 1: Formula for the Induced E.M.F.
The induced e.m.f. \( e \) due to the motion of the aeroplane in Earth's magnetic field is given by:
\[
e = B L v \sin \theta
\]
where:
- \( B \) is the magnetic field strength,
- \( L \) is the wingspan of the aeroplane,
- \( v \) is the velocity of the aeroplane, and
- \( \theta \) is the angle of dip (the angle between the magnetic field and the horizontal).
Step 2: Horizontal Component of the Magnetic Field.
The horizontal component of Earth's magnetic field is \( H \), so we have:
\[
B = H
\]
Step 3: Substituting into the Formula.
The induced e.m.f. becomes:
\[
e = H L v \sin \theta
\]
Step 4: Solving for \( \theta \).
Rearranging the above equation to solve for \( \theta \), we get:
\[
\sin \theta = \frac{e}{H L v}
\]
Thus, the expression for the angle of dip \( \theta \) is:
\[
\theta = \sin^{-1} \left( \frac{e}{H L v} \right)
\]
Step 5: Conclusion.
Thus, the angle of dip at the place is given by:
\[
\boxed{\theta = \sin^{-1} \left( \frac{e}{H L v} \right)}
\]