Which transition in the hydrogen spectrum would have the same wavelength as the Balmer type transition from $n =4$ to $n =2$ of $He ^{+}$spectrum
\[ \frac{1}{\lambda(H)} = R(1)^2 \left( \frac{1}{n_1^2} - \frac{1}{n_2^2} \right) \]
where \( R(1) \) is the Rydberg constant for hydrogen. For He\(^{+}\), the formula is:\[ \frac{1}{\lambda(\text{He}^+)} = R(2)^2 \left( \frac{1}{2^2} - \frac{1}{4^2} \right) \]
Given \( \lambda(H) = \lambda(\text{He}^+) \), we equate the two equations:\[ R(1)^2 \left( \frac{1}{n_1^2} - \frac{1}{n_2^2} \right) = R(2)^2 \left( \frac{1}{2^2} - \frac{1}{4^2} \right) \]
Simplifying and comparing \( n_1 = 1 \) and \( n_2 = 2 \), we find the correct transition in the hydrogen spectrum is from \( n = 2 \) to \( n = 1 \). Thus, the correct answer is option (1).What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)

Cobalt chloride when dissolved in water forms pink colored complex $X$ which has octahedral geometry. This solution on treating with cone $HCl$ forms deep blue complex, $\underline{Y}$ which has a $\underline{Z}$ geometry $X, Y$ and $Z$, respectively, are
What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,
The atomic structure of an element refers to the constitution of its nucleus and the arrangement of the electrons around it. Primarily, the atomic structure of matter is made up of protons, electrons and neutrons.
Dalton proposed that every matter is composed of atoms that are indivisible and indestructible.
The following are the postulates of his theory:
Several atomic structures of an element can exist, which differ in the total number of nucleons.These variants of elements having a different nucleon number (also known as the mass number) are called isotopes of the element. Therefore, the isotopes of an element have the same number of protons but differ in the number of neutrons. For example, there exist three known naturally occurring isotopes of hydrogen, namely, protium, deuterium, and tritium.