Chapter 14: Problem 44
A car horn emits \(380-\mathrm{Hz}\) sound. If the car moves at \(17 \mathrm{m} / \mathrm{s}\) with its horn blasting, what frequency will a person standing in front of the car hear?
Short Answer
Expert verified
The person standing in front of the car will hear a frequency of 400 Hz.
Step by step solution
01
Understand the Doppler effect
The Doppler effect is a change in the observed frequency of a wave when the observer and source are in motion relative to each other. Formula for observed frequency when the source is moving towards the observer in sound is: \(f_o = f_s \frac{v + v_o}{v + v_s}\), where, \(f_o\) is observed frequency, \(f_s\) is source frequency, \(v\) is speed of sound in air, \(v_o\) is speed of observer, and \(v_s\) is speed of source.
02
Identify the known variables
From the problem, we are given the following: source frequency (\(f_s\)) which is the car horn's frequency = 380 Hz, speed of the car (\(v_s\)) = 17 m/s, speed of sound in air (v) = 343 m/s. Since the person is standing still, the speed of observer (\(v_o\)) = 0.
03
Plug the values into the formula
We can substitute the known values into the formula \(f_o = f_s \frac{v + v_o}{v - v_s}\), which becomes \(f_o = 380 \frac{343 + 0}{343 - 17}\)
04
Do the calculations
Calculate the fractions and subtract inside the denominator, then multiply with source frequency (380 Hz). This results in \(f_o = 380 \times \frac{343}{326}\)
05
Round-up the resultant frequency
Calculate the product to get the observed frequency. Rounding up to nearest whole number gives us 400 Hz
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Observed Frequency Calculation
The Doppler effect is a fascinating phenomenon that occurs when there is a relative movement between a wave source and an observer. To calculate the observed frequency, which is the frequency detected by the observer, we use a specific formula that takes into account this relative movement.
When the source is moving towards the observer, the waves seem to 'compress,' and the frequency appears higher. Conversely, when the source is moving away, the waves 'stretch,' making the frequency seem lower. This change in perceived frequency is quantifiable and key to calculating the observed frequency. For a sound source moving towards a stationary observer, the formula is:
\[\begin{equation}f_o = f_s \frac{v + v_o}{v - v_s}\end{equation}\]
where,
When the source is moving towards the observer, the waves seem to 'compress,' and the frequency appears higher. Conversely, when the source is moving away, the waves 'stretch,' making the frequency seem lower. This change in perceived frequency is quantifiable and key to calculating the observed frequency. For a sound source moving towards a stationary observer, the formula is:
\[\begin{equation}f_o = f_s \frac{v + v_o}{v - v_s}\end{equation}\]
where,
- \(f_o\) is the observed frequency,
- \(f_s\) is the source frequency,
- \(v\) is the speed of sound in air,
- \(v_o\) is the observer's velocity, and
- \(v_s\) is the source's velocity.
Sound Wave Frequency
Sound waves, like any other waves, have a frequency, which is the number of waves that pass a point in a certain period of time. The frequency of a sound wave determines its pitch; the higher the frequency, the higher the pitch. The unit of frequency is hertz (Hz), which equates to one wave per second.
The source frequency in our exercise is the frequency at which the car horn emits sound (380 Hz). This frequency is a characteristic of the sound source itself and remains constant regardless of the motion of the source, but the frequency observed by an individual can vary due to the relative motion between them and the source. It's this interplay of source frequency and relative motion that's at the heart of the Doppler effect and why the observed frequency can differ from the source frequency.
The source frequency in our exercise is the frequency at which the car horn emits sound (380 Hz). This frequency is a characteristic of the sound source itself and remains constant regardless of the motion of the source, but the frequency observed by an individual can vary due to the relative motion between them and the source. It's this interplay of source frequency and relative motion that's at the heart of the Doppler effect and why the observed frequency can differ from the source frequency.
Relative Motion in Wave Propagation
Relative motion is a core concept when discussing wave propagation, especially in the context of the Doppler effect. It refers to the movement of the wave source in relation to the observer.
When considering sound waves, if the source of the sound is moving towards you, the waves are reaching you more frequently than if the source were stationary, leading to a higher frequency or pitch. If the source moves away, it's the opposite—the waves are spread out, and the observed frequency or pitch is lower. This effect is not only observed with sound but with all types of waves, including light waves, which is why it's such a fundamental concept in wave physics.
When considering sound waves, if the source of the sound is moving towards you, the waves are reaching you more frequently than if the source were stationary, leading to a higher frequency or pitch. If the source moves away, it's the opposite—the waves are spread out, and the observed frequency or pitch is lower. This effect is not only observed with sound but with all types of waves, including light waves, which is why it's such a fundamental concept in wave physics.