Step 1: Use the Bragg's law.
Bragg’s law for diffraction is given by
\[
n \lambda = 2 d \sin \theta,
\]
where \( n \) is the diffraction order, \( \lambda \) is the wavelength, \( d \) is the distance between the planes, and \( \theta \) is the diffraction angle.
Step 2: Calculate the distance between planes.
The lattice parameter \( a = 3.61 \, \text{Å} \) and for the \( \{ 1 1 0 \} \) planes,
\[
d = \frac{a}{\sqrt{h^2 + k^2 + l^2}} = \frac{3.61}{\sqrt{1^2 + 1^2 + 0^2}} = \frac{3.61}{\sqrt{2}} = 2.55 \, \text{Å}.
\]
Step 3: Apply Bragg’s law for maximum diffraction order.
For the highest order diffraction, \( \theta = 90^\circ \), so
\[
n = \frac{2 d}{\lambda}.
\]
Substitute the values \( d = 2.55 \, \text{Å} \) and \( \lambda = 0.090 \, \text{nm} = 0.090 \times 10^{-1} \, \text{Å} \):
\[
n = \frac{2 \times 2.55}{0.090} \approx 56.67.
\]
Thus, the highest integer \( n \) is 56.
Final Answer: The highest order present in the diffraction pattern is \( \boxed{56}. \)