Step 1: De Broglie Condition
Circumference = nλ
$2 \pi r = n \lambda$
Step 2: De Broglie Wavelength
$\lambda = \frac{h}{mv}$
Step 3: Substitute λ in Step 1
$2 \pi r = n \frac{h}{mv}$
Step 4: Electrostatic Force = Centripetal Force
$\frac{1}{4\pi\epsilon_0} \frac{e^2}{r^2} = \frac{mv^2}{r}$
$v^2 = \frac{e^2}{4\pi\epsilon_0 mr}$
Step 5: Express v
$v = \frac{e}{\sqrt{4\pi\epsilon_0 mr}}$
Step 6: Substitute v in Step 3
$2 \pi r = n \frac{h}{m \frac{e}{\sqrt{4\pi\epsilon_0 mr}}}$
$2 \pi r = n \frac{h \sqrt{4\pi\epsilon_0 mr}}{me}$
Step 7: Solve for r
$r^{1/2} = n \frac{h \sqrt{4\pi\epsilon_0 m}}{2\pi me}$
$r = n^2 \frac{h^2 4\pi\epsilon_0 m}{(2\pi me)^2} = \frac{n^2 h^2 \epsilon_0}{\pi m e^2}$
Step 8: Determine n from figure
Count wavelengths in circumference, $n=3$.
Step 9: Substitute n=3 in r
$r = \frac{3^2 h^2 \epsilon_0}{\pi m e^2} = \frac{9 h^2 \epsilon_0}{\pi m e^2}$
Final Answer: The final answer is $\frac{9 h^2 \epsilon_0}{\pi m e^2}$
The de Broglie wavelength for the electron is given by:
$\lambda = \frac{h}{mv}$
For standing waves, the circumference of the orbit must be an integer multiple of the wavelength. Therefore, the condition for the orbit radius $r$ is:
$2\pi r = n \lambda$
Substituting for the de Broglie wavelength $\lambda$, we get:
$2\pi r = n \frac{h}{mv}$
This leads to an expression for the radius in terms of fundamental constants, and for the ground state (where $n = 1$), the radius is given by:
$r = \frac{9h^2 \epsilon_0}{\pi m e^2}$
Thus, the correct expression for the orbit radius is option $r = \frac{9h^2 \epsilon_0}{\pi m e^2}$.
A block of certain mass is placed on a rough floor. The coefficients of static and kinetic friction between the block and the floor are 0.4 and 0.25 respectively. A constant horizontal force \( F = 20 \, \text{N} \) acts on it so that the velocity of the block varies with time according to the following graph. The mass of the block is nearly (Take \( g = 10 \, \text{m/s}^2 \)):
A wooden block of mass M lies on a rough floor. Another wooden block of the same mass is hanging from the point O through strings as shown in the figure. To achieve equilibrium, the coefficient of static friction between the block on the floor and the floor itself is