Constructive interference from parallel crystal planes obeys the Bragg condition $2d\sin\theta = n\lambda$, with $n=1$ for the first observed reflection.
Here the path difference between rays scattered off successive planes equals one wavelength. Solving for $d$ gives $d = \dfrac{\lambda}{2\sin\theta}$ for first order.
Substitute $\lambda = 0.16\ \text{nm}$ and $\theta = 30^\circ$. Since $\sin 30^\circ = 1/2$, the factor $2\sin\theta = 2 \times 0.5 = 1$.
Therefore $d = \dfrac{0.16\ \text{nm}}{1} = 0.16\ \text{nm}$. The spacing happens to equal the wavelength here because $2\sin\theta = 1$ exactly at this angle.
\[\boxed{d = 0.16\ \text{nm}}\]