The de-Broglie wavelength $\lambda$ is given by:
\[\lambda = \frac{h}{mv}\]
For an electron in motion:
\[\text{Kinetic Energy (K.E.)} = \frac{1}{2} mv^2 \implies v^2 = \frac{2 \cdot \text{K.E.}}{m}.\]
Step 1: Substituting values:
\[\text{K.E.} = R_H = 2.18 \times 10^{-18} \, \text{J}.\]
\[v = \sqrt{\frac{2 \cdot R_H}{m}} = \sqrt{\frac{2 \cdot 2.18 \times 10^{-18}}{9.1 \times 10^{-31}}}.\]
Step 2: Using frequency relation:
\[\nu = \frac{v}{\lambda} = \frac{h}{mv}.\]
Step 3: Substituting $h$ and solving for $\nu$:
\[\nu = \frac{\text{K.E.}}{h} = \frac{2.18 \times 10^{-18}}{6.6 \times 10^{-34}}.\]
\[\nu = 660.6 \times 10^{13} \, \text{Hz}.\]
Step 4: Nearest integer:
\[\nu \approx 661 \times 10^{13} \, \text{Hz}\]
The problem asks for the frequency of the de-Broglie wave associated with an electron in the first Bohr orbit of a hydrogen atom.
The term "frequency of the de-Broglie wave" can be interpreted in the context of the Bohr model as the classical frequency of revolution of the electron in its orbit. The de-Broglie wave for a stable orbit forms a standing wave, and its properties are intrinsically linked to the dynamics of the orbiting electron.
The frequency of revolution (\(f\)) for an electron in the n-th Bohr orbit of a hydrogen atom is given by the formula:
\[ f_n = \frac{2 R_H}{h n^3} \]where:
This formula can be derived from the expression for the total energy of the electron, \(E_n = -R_H/n^2\), and classical mechanics relationships for circular motion under a Coulomb force.
Step 1: Identify the given values and the specific orbit.
Step 2: Substitute the given values into the formula for the frequency of revolution.
We use the formula \(f_n = \frac{2 R_H}{h n^3}\) with \(n=1\):
\[ f_1 = \frac{2 R_H}{h (1)^3} = \frac{2 R_H}{h} \]Step 3: Perform the calculation.
\[ f_1 = \frac{2 \times (2.18 \times 10^{-18} \, \text{J})}{6.6 \times 10^{-34} \, \text{J.s}} \] \[ f_1 = \frac{4.36 \times 10^{-18}}{6.6 \times 10^{-34}} \, \text{Hz} \] \[ f_1 \approx 0.6606 \times 10^{16} \, \text{Hz} \] \[ f_1 = 6.606 \times 10^{15} \, \text{Hz} \]The problem asks for the frequency to be expressed in the format ______ \( \times 10^{13} \, \text{Hz} \).
We need to convert our calculated frequency to this format:
\[ f_1 = 6.606 \times 10^{15} \, \text{Hz} = 660.6 \times 10^{13} \, \text{Hz} \]Rounding this value to the nearest integer, we get 661.
The frequency of the de-Broglie wave is 661 \( \times 10^{13} \, \text{Hz} \).
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,