\( 340 \) Hz
Step 1: Relationship between path difference and phase difference
The phase difference \( \Delta \phi \) and path difference \( \Delta x \) of a wave are related by: \[ \Delta \phi = \frac{2\pi}{\lambda} \Delta x \] Given: \[ \Delta \phi = 1.8\pi, \quad \Delta x = 50 \text{ cm} = 0.50 \text{ m} \] Step 2: Solve for wavelength \( \lambda \)
Rearranging the equation: \[ \lambda = \frac{2\pi \times 0.50}{1.8\pi} \] \[ \lambda = \frac{1.0}{1.8} = 0.555 \text{ m} \] Step 3: Calculate frequency
The frequency of a wave is given by: \[ f = \frac{v}{\lambda} \] where \( v = 340 \) m/s is the speed of sound in air. \[ f = \frac{340}{0.555} \] \[ f \approx 612 \text{ Hz} \] Thus, the frequency of the sound wave is \( 612 \) Hz.
Wave picture of light has failed to explain
(1) photoelectric effect
(2) interference of light
(3) diffraction of light
(4) polarization of light
If the function
\[ f(x) = \begin{cases} \frac{(e^x - 1) \sin kx}{4 \tan x}, & x \neq 0 \\ P, & x = 0 \end{cases} \]
is differentiable at \( x = 0 \), then:
If
\[ A = \{ P(\alpha, \beta) \mid \text{the tangent drawn at P to the curve } y^3 - 3xy + 2 = 0 \text{ is a horizontal line} \} \]
and
\[ B = \{ Q(a, b) \mid \text{the tangent drawn at Q to the curve } y^3 - 3xy + 2 = 0 \text{ is a vertical line} \} \]
then \( n(A) + n(B) = \)