Respuesta :
Answer:
(a) Approximately 968 Hz.
Explanation:
The observed frequency is less than 1003 Hz because of Doppler's Effect. When the source is moving away from an observer that doesn't move, the equation for the observed frequency [tex]f_\text{observed}[/tex] would be:
[tex]f_\text{observed} = \displaystyle \frac{c}{c + v_\text{source}} \cdot f_\text{source}[/tex],
where in the context of this problem,
- [tex]c = 334\; \rm m \cdot s^{-1}[/tex] is the speed of sound in the air.
- [tex]v_\text{source} = 12.0\; \rm m \cdot s^{-1}[/tex] is the speed at which the source moves away from the observer.
- [tex]f_\text{source} = 1003\; \rm Hz[/tex] is the frequency at the source.
Apply this equation to find [tex]f_\text{observed}[/tex]:
[tex]\begin{aligned}f_\text{observed} &= \frac{c}{c + v_\text{source}} \cdot f_\text{source} \\ &= \frac{334}{334 + 12.0} \times 1003 \\ &\approx 968\; \rm Hz\end{aligned}[/tex].
Here's an alternative explanation.
The frequency of the siren at the source is [tex]f = 1003\; \rm Hz[/tex]. That corresponds to a period of [tex]T = \displaystyle \frac{1}{f} \approx 9.97\times 10^{-4}\; \rm s[/tex].
In other words, at the source, a peak arrives about every [tex]9.97\times 10^{-4}\; \rm s[/tex].
The source is moving away from the observer at a speed of [tex]v = 12.0\; \rm m \cdot s^{-1}[/tex]. In the [tex]9.97\times 10^{-4}\; \rm s[/tex] between the first and the second peak, the source moved [tex]9.97 \times 10^{-4} \times 12.0 \approx 0.011964\; \rm m[/tex] away from the observer. It would take an extra [tex]\displaystyle \frac{0.011964\; \rm m}{334\; \rm m \cdot s^{-1}} \approx 3.58 \times 10^{-5}\; \rm s[/tex] for the sound to cover that extra distance.
As a result, the period of the sound would appear to be [tex]9.97\times 10^{-4} + 3.58 \times 10^{-5} \approx 1.03 \times 10^{-3} \; \rm s[/tex] to the observer.
That corresponds to an observed frequency of [tex]\displaystyle \frac{1}{1.03 \times 10^{-3}} \approx 968\; \rm Hz[/tex]. (Same as the answer from the formula.)