Step 1: Relate the components of the Earth's magnetic field.
Let $B$ be the total intensity of the Earth's magnetic field.
Let $B_H$ be the horizontal component and $B_V$ be the vertical component.
The total field is the vector sum of its components:
\[
B^2 = B_H^2 + B_V^2.
\]
The angle of dip, $\delta$, is the angle between the total field and the horizontal component, defined by:
\[
\tan\delta = \frac{B_V}{B_H}.
\]
Step 2: Use the given condition to find the ratio of components.
We are given that the Earth's magnetic field is twice its vertical component:
\[
B = 2 B_V.
\]
Substitute this into the total field equation:
\[
(2 B_V)^2 = B_H^2 + B_V^2.
\]
\[
4 B_V^2 = B_H^2 + B_V^2.
\]
\[
B_H^2 = 4 B_V^2 - B_V^2 = 3 B_V^2.
\]
Step 3: Find the relationship between $B_H$ and $B_V$.
Take the square root of the equation from Step 2:
\[
B_H = \sqrt{3} B_V.
\]
Step 4: Calculate the required ratio.
The question asks for the ratio of the horizontal component to the total magnetic field, $\frac{B_H}{B}$.
From the given information, we have $B = 2 B_V$ and $B_V = \frac{1}{\sqrt{3}} B_H$.
Substitute $B_V$ in the first relation:
\[
B = 2 \left(\frac{1}{\sqrt{3}} B_H\right) = \frac{2}{\sqrt{3}} B_H.
\]
Rearrange to find the ratio $\frac{B_H}{B}$:
\[
\frac{B_H}{B} = \frac{\sqrt{3}}{2}.
\]
The ratio is $\sqrt{3}:2$.