Assertion A states that the Bohr model is applicable to hydrogen and hydrogen-like atoms only.
Hydrogen-like atoms are those that have only one electron, such as \( He^+, Li^{2+}, Be^{3+} \), etc.
The Bohr model successfully explains the atomic spectra of hydrogen and these single-electron species.
For atoms with more than one electron, the Bohr model fails to predict the correct spectra.
Thus, Assertion A is true. Reason R states that the formulation of the Bohr model does not include the repulsive force between electrons.
The Bohr model is a simplified model of the atom that considers electrons orbiting the nucleus in specific quantized energy levels.
It does not take into account the inter-electronic repulsions that are significant in multi-electron atoms.
The absence of consideration for electron-electron repulsion is a primary reason why the Bohr model is only accurate for single-electron systems. Thus, Reason R is also true. Furthermore, the reason R correctly explains why the Bohr model is limited to hydrogen and hydrogen-like atoms. The simplicity of having only one electron eliminates the complexities arising from electron-electron interactions, which are not accounted for in the Bohr model. Therefore, Reason R is the correct explanation of Assertion A.
Let \( T_r \) be the \( r^{\text{th}} \) term of an A.P. If for some \( m \), \( T_m = \dfrac{1}{25} \), \( T_{25} = \dfrac{1}{20} \), and \( \displaystyle\sum_{r=1}^{25} T_r = 13 \), then \( 5m \displaystyle\sum_{r=m}^{2m} T_r \) is equal to:
The largest $ n \in \mathbb{N} $ such that $ 3^n $ divides 50! is: