Step 1: Set up the geometry.
Two identical magnets sit on the same line with their centres $0.2$ m apart. The midpoint is halfway, so each magnet is a distance $d = 0.1$ m from it. Their axes are perpendicular to each other.
Step 2: Recall the two field formulas.
For a short magnet of moment $M$ at distance $d$, the field on its axis is $\dfrac{\mu_0}{4\pi}\dfrac{2M}{d^{3}}$ and on its equator is $\dfrac{\mu_0}{4\pi}\dfrac{M}{d^{3}}$. The midpoint is on the axis of one magnet and on the equator of the other.
Step 3: Compute the base field.
Let $B_0 = \dfrac{\mu_0}{4\pi}\dfrac{M}{d^{3}}$. With $\dfrac{\mu_0}{4\pi} = 10^{-7}$, $M = 10$, $d = 0.1$: \[ B_0 = 10^{-7}\times\frac{10}{(0.1)^{3}} = 10^{-7}\times10^{4} = 10^{-3}\ \text{T} \]
Step 4: Write the two fields.
The axial field is $B_1 = 2B_0$ and the equatorial field is $B_2 = B_0$.
Step 5: Add the perpendicular fields.
Since the two fields are at right angles, combine them with the Pythagoras rule: \[ B_{net} = \sqrt{(2B_0)^{2} + B_0^{2}} = \sqrt{5}\,B_0 \]
Step 6: Put the value in.
\[ B_{net} = \sqrt{5}\times10^{-3}\ \text{T} \] \[ \boxed{B_{net} = \sqrt{5}\times10^{-3}\ \text{T}} \]