As shown in the figure, X-ray diffraction pattern is obtained from a diatomic chain of atoms P and Q. The diffraction condition is given by \( a \cos \theta = n\lambda \), where \( n \) is the order of the diffraction peak. Here, \( a \) is the lattice constant and \( \lambda \) is the wavelength of the X-rays. Assume that atomic form factors and resolution of the instrument do not depend on \( \theta \). Then, the intensity of the diffraction peaks is 
To solve this problem, we need to analyze the diffraction pattern from a diatomic chain of atoms using the given condition:
\(a \cos \theta = n\lambda\)
where \(a\) is the lattice constant, \(n\) is the order of the diffraction peak, \(\theta\) is the angle, and \(\lambda\) is the wavelength of the X-rays.
For a diatomic chain composed of two different atoms, P and Q, the intensity of the diffraction peaks depends on the basis of the lattice. In general, for such a diatomic chain, the diffraction condition will lead to different intensities for different orders of peaks. This is because the scattering factors of the atoms (P and Q) can lead to constructive or destructive interference.
Let's analyze the intensity pattern:
This means that the intensity of diffraction peaks is indeed lower for odd values of \(n\) compared to even values of \(n\).
Hence, the correct answer is:
lower for odd values of \(n\), when compared to even values of \(n\)
The figure shows an opamp circuit with a 5.1 V Zener diode in the feedback loop. The opamp runs from \( \pm 15 \, {V} \) supplies. If a \( +1 \, {V} \) signal is applied at the input, the output voltage (rounded off to one decimal place) is:
A wheel of mass \( 4M \) and radius \( R \) is made of a thin uniform distribution of mass \( 3M \) at the rim and a point mass \( M \) at the center. The spokes of the wheel are massless. The center of mass of the wheel is connected to a horizontal massless rod of length \( 2R \), with one end fixed at \( O \), as shown in the figure. The wheel rolls without slipping on horizontal ground with angular speed \( \Omega \). If \( \vec{L} \) is the total angular momentum of the wheel about \( O \), then the magnitude \( \left| \frac{d\vec{L}}{dt} \right| = N(MR^2 \Omega^2) \). The value of \( N \) (in integer) is:
In the transistor circuit shown in the figure, \( V_{BE} = 0.7 \, {V} \) and \( \beta_{DC} = 400 \). The value of the base current in \( \mu A \) (rounded off to one decimal place) is: