Doppler-shifted frequency problem

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Also, please provide a link to the original problem so we can see what the specific questions are. This summary is not a complete answer to the questions given.
  • #1
hitman0097
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Homework Statement


A radar "speed gun" emits microwaves of frequency fo=36.0 GHz. When the gun is pointed at an object moving toward it at speed v, the object senses the microwaves at the Doppler-shifted frequency f. The moving object reflects these microwaves at this same frequency f. The stationary radar apparatus detects these reflected waves at a Doppler-shifted f'. The gun combines its emitted wave at fo and its detected wave at f'. These waves interfere, creating a beat pattern whose beat frequency is fbeat=f'-fo.

a.) Show that: v≈cfbeat/2fo,

if fbeat <<fo. If fbeat=6670 Hz, what is v(km/h)?

b.) If the object's speed is different by v, show that the difference in in beat frequency Δfbeat is given by : Δfbeat=2foΔv / c

c.) If the accuracy of the speed gun is to be 1 km/h, to what accuracy must the beat frequency be measured?

Homework Equations


f=c/λ = fo[(c+v/c-v)^1/2]
λ=λo[(c-v/c+v)^1/2]
1/foo/c

The Attempt at a Solution


I am kind of lost on this problem, I think I heard my teacher say I'd need a double doppler shift. Any help and hints are appreciated!

Thanks
 
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  • #2
The first Doppler shift that occurs should be in the form
[ f=36.0 G hz [(c+v)/(c-v)]^.5]

The 2nd Doppler shift would be in the form of the first Doppler shift
[ f'=(f [(c+v/c-v)]^.5)] = 36 Ghz [(c+v)/(c-v)]

fbeat can be related in terms of f not [fbeat = 36.0 Ghz [(c+v)/(c-v)] - 36.0 Ghz]
 
  • #3
Still confused to as v= c (fbeat)/ 2 fo If: fbeat<<fo. Also, I think the last fbeat is not correctly expressed or related by me. Also getting getting 27.34 m/s for part (a). Where the answer in the back of my book is 1.00 x 10^2 km/hr
 
  • #4
There is no difference between the moving-source and moving-observer doppler-shift expressions for light. For waves that need a medium, the wave-speed gets measured wrt the medium which is why there is a difference there.

The usual idea is that a moving car reflects the waves as it receives them - so the reflected wavelength is shifted wrt the transmitted one.
The vehicle then acts as a source for the reflected wave.

https://www.physicsforums.com/showthread.php?t=223186
... subs in water - sonar doppler-shift illustrating the double-shift.

https://www.physicsforums.com/archive/index.php/t-335219.html
... for radar gun!

Not following your reasoning - what is the relationship between the beat frequency and the doppler shifted frequency?
We need to see how you are getting these results in order to help you properly.
 
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  • #5
for reaching out. It sounds like your teacher may have been referring to the Doppler effect, which is the change in frequency of a wave due to the relative motion between the source of the wave and the observer. In this problem, the radar "speed gun" is the source of the microwaves and the moving object is the observer.

To find the speed of the object, we can use the equation v=λf, where v is the speed of the object, λ is the wavelength of the waves, and f is the frequency of the waves. We can also use the Doppler effect equation, f'=f(v/c+v)/(c-v), where f' is the frequency detected by the radar apparatus, f is the emitted frequency, v is the speed of the object, and c is the speed of light.

For part a), we are given the beat frequency, fbeat, and we want to find the speed of the object, v. We can rearrange the Doppler effect equation to solve for v, giving us v=c(fbeat/2fo). Since we are given the beat frequency in Hz, we need to convert it to m/s by multiplying by the speed of light, c=3.0x10^8 m/s. We also need to convert the emitted frequency, fo, from GHz to Hz by multiplying by 10^9. Plugging in these values, we get v≈cfbeat/2fo≈3.0x10^8 m/s x 6670 Hz/(2x36.0x10^9 Hz)≈34.8 m/s.

To convert this to km/h, we can multiply by 3.6, giving us v≈125 km/h.

For part b), we need to find the difference in beat frequency, Δfbeat, when the speed of the object changes by Δv. We can use the same equation for v as before, but now we have two different speeds, v and v+Δv. Plugging these values into the equation, we get Δfbeat=2fo((v+Δv)/c)/(c-(v+Δv)) - 2fo(v/c)/(c-v). Simplifying this expression, we get Δfbeat=2foΔv/c(c-v). Again, we need to convert the emitted frequency, fo, from GHz to Hz by multiplying by 10^9. Pl
 

Related to Doppler-shifted frequency problem

1. What is the Doppler-shifted frequency problem?

The Doppler-shifted frequency problem is a phenomenon in which the frequency of a wave changes as the source of the wave moves relative to the observer. This is commonly observed in sound and light waves, and can result in a higher or lower perceived frequency depending on the direction of movement.

2. How does the Doppler-shifted frequency problem occur?

The Doppler-shifted frequency problem occurs due to the relative motion between the source of a wave and the observer. As the source moves towards the observer, the wave is compressed, resulting in a higher frequency. Conversely, as the source moves away from the observer, the wave is stretched, resulting in a lower frequency.

3. What are some real-world applications of the Doppler-shifted frequency problem?

The Doppler-shifted frequency problem has many practical applications, such as in radar and sonar technology, where it is used to measure the speed and direction of moving objects. It is also used in medical imaging, such as ultrasound, to detect the movement of blood in the body.

4. How is the Doppler-shifted frequency problem calculated?

The Doppler-shifted frequency problem can be calculated using the Doppler effect equation, which takes into account the relative velocity between the source and observer, as well as the speed of the wave. This equation can be used to determine the change in frequency observed by the observer.

5. How can the Doppler-shifted frequency problem be minimized in practical applications?

In practical applications, the Doppler-shifted frequency problem can be minimized by using techniques such as frequency modulation. This involves varying the frequency of the wave in a controlled manner, which can help to reduce the impact of the Doppler effect. Additionally, using higher frequencies can also help to minimize the effects of the Doppler-shifted frequency problem.

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