A policeman with a very good ear and a good understanding of the Doppler effect stands on the shoulder of a freeway assisting a crew in a 40 -mph work zone. He notices a car approaching that is honking its horn. As the car gets closer, the policeman hears the sound of the horn as a distinct \(\mathrm{B} 4\) tone \((494 \mathrm{~Hz}) .\) The instant the car passes by, he hears the sound as a distinct \(\mathrm{A} 4\) tone \((440 \mathrm{~Hz}) .\) He immediately jumps on his motorcycle, stops the car, and gives the motorist a speeding ticket. Explain his reasoning.

Short Answer

Expert verified
Answer: Yes, the motorist was speeding at 126.62 mph, which is significantly higher than the 40 mph speed limit in the work zone.

Step by step solution

01

Understand the Doppler effect formula

The Doppler effect formula is given by: \(f' = f \frac{v + v_{0}}{v + v_{s}}\) where \(f'\) is the frequency observed by the listener (policeman), \(f\) is the source frequency (car's honk), \(v\) is the speed of sound, \(v_{0}\) is the speed of the listener relative to the air (usually 0 for a stationary listener), and \(v_{s}\) is the speed of the source relative to the air.
02

Set up the equations for approaching and passing frequencies

Now, we can set up two separate equations for when the car is approaching and when it passes the policeman. As the car approaches, the observed frequency is higher (494 Hz), and as it passes, the observed frequency is lower (440 Hz). For approaching: \(f' = f \frac{v}{v - v_{s}}\) For passing: \(f' = f \frac{v}{v + v_{s}}\)
03

Solve for the car's speed, \(v_s\)

Now, we can solve for \(v_s\). First, we will need to find the ratio of approaching to passing frequencies, which is \(\frac{494}{440}\). Then, we can write the following equation: \(\frac{v}{v - v_{s}} = \frac{494}{440}\frac{v}{v + v_{s}}\) Next, we will solve this equation for \(v_s\). First, multiply both sides by \((v-v_s)(v+v_s)\) to get: \(v(v + v_{s})(v - v_{s}) = \frac{494}{440}(v + v_{s})(v - v_{s})(v)\) Now we can simplify this equation to: \(v_s^2 = \frac{494}{440}v^2 - v^2\) Let \(v\) be the typical speed of sound, about 343 m/s: \(v_s^2 = \frac{494}{440}(343^2) - 343^2\) Solving for \(v_s\): \(v_s = \sqrt{(\frac{494}{440})(343^2) - 343^2} = 56.62~\mathrm{m/s}\) Convert this to mph: \(v_s = 56.62 \cdot \frac{3600}{1609.34} = 126.62~\mathrm{mph}\)
04

Determine if the car was speeding

Now that we've calculated the speed of the car 126.62 mph, we can compare it to the speed limit in the work zone, which is 40 mph. Since the car's speed is much higher than the speed limit, the policeman's decision to give the motorist a speeding ticket is justified.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

A half-open pipe is constructed to produce a fundamental frequency of \(262 \mathrm{~Hz}\) when the air temperature is \(22^{\circ} \mathrm{C} .\) It is used in an overheated building when the temperature is \(35^{\circ} \mathrm{C} .\) Neglecting thermal expansion in the pipe, what frequency will be heard?

Two trains are traveling toward each other in still air at \(25.0 \mathrm{~m} / \mathrm{s}\) relative to the ground. One train is blowing a whistle at \(300 .\) Hz. The speed of sound is \(343 \mathrm{~m} / \mathrm{s}\). a) What frequency is heard by a man on the ground facing the whistle-blowing train? b) What frequency is heard by a man on the other train?

When two pure tones with similar frequencies combine to produce beats, the result is a train of wave packets. That is, the sinusoidal waves are partially localized into packets. Suppose two sinusoidal waves of equal amplitude A, traveling in the same direction, have wave numbers \(\kappa\) and \(\kappa+\Delta \kappa\) and angular frequencies \(\omega\) and \(\omega+\Delta \omega\), respectively. Let \(\Delta x\) be the length of a wave packet, that is, the distance between two nodes of the envelope of the combined sine functions. What is the value of the product \(\Delta x \Delta \kappa ?\)

If you blow air across the mouth of an empty soda bottle, you hear a tone. Why is it that if you put some water in the bottle, the pitch of the tone increases?

At a state championship high school football game, the intensity level of the shout of a single person in the stands at the center of the field is about \(50 \mathrm{~dB}\). What would be the intensity level at the center of the field if all 10,000 fans at the game shouted from roughly the same distance away from that center point?

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free