\( 2:3 \)
Step 1: Applying the Doppler effect formula
The observed frequency when the observer is moving away from the stationary source is given by: \[ f' = f \times \frac{v}{v + v_o} \] where: - \( f = 102 \) Hz (source frequency), - \( v \) is the speed of sound in air, - \( v_o = 0.1 v \) (observer’s speed moving away).
Step 2: Compute the observed frequencies
For observer 1 moving away: \[ f'_1 = 102 \times \frac{v}{v + 0.1v} \] \[ = 102 \times \frac{v}{1.1v} \] \[ = 102 \times \frac{1}{1.1} \] \[ \approx 92.7 \text{ Hz} \] For observer 2 moving in the opposite direction, the same calculation applies: \[ f'_2 = 102 \times \frac{v}{1.1v} = 92.7 \text{ Hz} \]
Step 3: Find the ratio of frequencies
\[ \frac{f'_1}{f'_2} = \frac{92.7}{92.7} = 1:1 \] Thus, the ratio of the frequencies of sound heard by the observers is \( 1:1 \).
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 \( n(A) + n(B) = \)