(110)
The position of diffraction peaks in an X-ray powder pattern depends on the interplanar spacing ($d_{hkl}$) via Bragg's Law. For cubic crystals, $d_{hkl}$ is related to the Miller indices ($hkl$) and lattice constant ($a$) by:
$d_{hkl} = \frac{a}{\sqrt{h^2 + k^2 + l^2}}$
Peaks appear in order of increasing $h^2 + k^2 + l^2$ values for simple cubic lattices, as this value dictates the spacing. We examine the lowest index planes:
Thus, the 2nd peak in the X-ray powder pattern of a simple cubic crystal is associated with the (110) plane.
A schematic of X-ray diffraction pattern of a single phase cubic polycrystal is given below. The miller indices of peak A is

In a powder diffraction experiment on BCC iron, the first peak occurs at $2\theta = 68.7^\circ$. The wavelength of X-rays is ________ (in nm to three decimal places).
Given: The lattice parameter of iron = $0.287 \text{ nm}$
X-ray diffraction pattern from an elemental metal with a FCC crystal structure shows the first peak at a Bragg angle $\theta = 24.65^\circ$. The lattice parameter of this metal is ____________ nm.
Given, wavelength of the X-ray used is $0.1543$ nm.