X-rays are ideal for determining crystal structures because their wavelengths (approximately 0.1–10 nm) match the interplanar spacing of crystal lattices. This enables constructive interference when X-rays interact with atoms in the crystal, following Bragg’s law:
\(n\lambda = 2d \sin \theta\)
where:
$n$: Order of diffraction.
$\lambda$: Wavelength of X-rays.
$d$: Interplanar spacing.
$\theta$: Angle of incidence.
The diffraction pattern generated by this interaction is analyzed to determine the atomic arrangement and symmetry in the crystal.
| List-I | List-II |
| (A) XeF2 | (iii) Linear |
| (B) BF3 | (i) Trigonal Planar |
| (C) XeF4 | (ii) Distorted Octahedral |
| (D) SF6 | (iv) Regular Octahedral |
| List-I | List-II |
|---|---|
| (A) Linus Pauling | (iii) Electronegativity |
| (B) Albert Einstein | (ii) Photoelectric effect |
| (C) Ernest Rutherford | (i) Alpha particle scattering experiment |
| (D) Max Planck | (iv) Black body radiations |
| List-I | List-II |
|---|---|
| (A) Lyman | (i) n = 2, 3, 4, ... |
| (B) Balmer | (ii) n = 3, 4, 5, ... |
| (C) Paschen | (iii) n = 4, 5, 6, ... |
| (D) Bracket | (iv) n = 5, 6, 7, ... |