What Is the Doppler Effect of an Ambulance Siren at Different Wind Conditions?

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Homework Help Overview

The discussion revolves around the Doppler Effect as it pertains to an ambulance siren, specifically analyzing how different wind conditions affect the frequency of the sound detected by an observer. The problem involves calculating the frequency ratios under calm conditions and with varying wind directions and speeds.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants explore the implications of wind direction on sound frequency, questioning the assumptions made about angles and reference frames. There is discussion about how to adjust velocities based on wind conditions and the geometry of the situation.

Discussion Status

Participants are actively engaging with the problem, offering various interpretations and calculations. There is a recognition of the complexity introduced by wind, with some guidance provided on how to approach the problem from different reference frames. Multiple interpretations of the wind's effect are being explored without a clear consensus on the correct approach.

Contextual Notes

Participants note the importance of understanding the wind's direction and its impact on sound velocity, as well as the need to clarify the assumptions regarding angles and reference frames. There is an acknowledgment of potential confusion regarding the effects of wind on sound propagation in different scenarios.

songoku
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Homework Statement


An ambulance is running on an expressway at a speed of 60 km/h from east to west (from A to B) with a siren of 880 Hz. Let the frequency of the siren sound detected by an observer located at a point O be Va and Vb when the vehicle just passes point A and point B respectively. Point C is just north of O and OC = AC = BC = 100 m. Here the sound velocity in calm air is 340 m/s.

a. In the case of calm weather (no wind), what is the approximate value of (Va / Vb) - 1
b. In the case of an east wind of 5 m/s, what is the approximate value of (Va / Vb) - 1
c. In the case of an north wind of 5 m/s, what is the approximate value of (Va / Vb) - 1

pic-1.jpg


Homework Equations



f ' = \frac{V sound \pm V observer}{V sound \mp Vsource} f

The Attempt at a Solution



Angle CAO = 45 degree
V source = 60 km/h cos 45 = 50/3 cos 45 m/s
V observer = 0

a. Va = \frac{340}{340 - 50/3 cos 45} 880

Vb = \frac{340}{340 + 50/3 cos 45} 880

(Va / Vb) - 1 = 0.07

b. Because east wind is from A to B as well, so V source = (50/3 + 5) cos 45 ?

c. Taking OA as x-axis, I break the velocity of north wind to other components and get the velocity along x-axis
V source = (50/3 - 5) cos 45 ?

thx
 
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Hi songoku. :smile:

There are a couple of questions regaring your problem statement. First, where did you get the angle of 45 degrees? It never specifically said so in the problem statement, so you may want to check that out. Assuming this is correct, however, let's take a look at parts b and c. It may be helpful to transform your reference frame so that the wind is at rest; that way you can use your formula. In the new reference frame for part b, the ambulance and the observer get a "boost" of 5 m/s in the negative x direction. Let me know if this works for you.
 
Hi Sam_Goldberg :)

About 45 degrees, I think that COA is an isosceles triangle because OC = AC. With angle OCA = 90 degrees, angle CAO = (180 - 90) / 2 = 45

To make the wind at rest, all the system is moving with velocity 5 m/s to the left ?

thx
 
songoku said:
About 45 degrees, I think that COA is an isosceles triangle because OC = AC. With angle OCA = 90 degrees, angle CAO = (180 - 90) / 2 = 45
Sounds correct to me.
 
For b, V source = (50/3 + 5) cos 45 and V observer = 5 cos 45 ?

Thx
 
Last edited:
I believe that those are the projections of the velocities onto AO (in m/s) in the frame of reference at rest w.r.t. the air, assuming that "east wind" blows toward the East (Usually, the wind direction is labeled as the direction where the wind is coming from).
 
turin said:
I believe that those are the projections of the velocities onto AO (in m/s) in the frame of reference at rest w.r.t. the air, assuming that "east wind" blows toward the East (Usually, the wind direction is labeled as the direction where the wind is coming from).

Yes, those are the projections of the velocities onto AO. But i think i get those values with assumption that east wind blows toward west, i.e. comes from east and moves to west, which is the wind moves from A to B.

I assume that all the system moves to the left with velocity 5m/s. Because the wind moves in the same direction as the ambulance, i think the velocity will increase and V source becomes (50/3 + 5) cos 45.

Then :
Va = \frac{340 + 5 cos 45}{340 - (50/3 + 5) cos 45} 880Vb = \frac{340 - 5 cos 45}{340 + (50/3 + 5) cos 45} 880

(Va / Vb) - 1 = 0.117

I know this is wrong because the answer is 0.07, but i don't know where my mistake is...

thx
 
You got it backward. If the wind moves in the same diretcion as the ambulance, then the speed of the ambulance in the air's rest frame is less. For instance, imagine that the ambulance is moving at the exact same speed as the wind, in the same direction. Then, what would be the speed of the ambulance in the air's rest frame? Would it be twice as much as the wind? (No.)
 
Oh now i get it.

And for (c), how to determine the effect of the wind?
I don't know because the wind is perpendicular to the direction of the ambulance..

thx
 
  • #10
Wind changes the velocity of the sound.
If wind moves in the direction of the sound, it adds up.
If it is in the opposite direction, it will decreases.
In this problem, the velocity of sound will increase with north wind, i.e wind blowing from north towards the observer.
When the wind is perpendicular to the sound velocity, it does not change
 
  • #11
rl.bhat said:
Wind changes the velocity of the sound.
If wind moves in the direction of the sound, it adds up.
If it is in the opposite direction, it will decreases.
In this problem, the velocity of sound will increase with north wind, i.e wind blowing from north towards the observer.
When the wind is perpendicular to the sound velocity, it does not change

So, for (b) the velocity of the sound will be 345 ?
 
  • #12
songoku said:
So, for (b) the velocity of the sound will be 345 ?
No. Due to east wind, the velocity of sound along AO will be 340 + 5cos45 and along BO will be 340 - 5cos45.
 
Last edited:
  • #13
and due to east wind, the speed of the ambulance will be (50/3 - 5) cos 45 and the speed of the observer will be 5 cos 45 along AO?

thx
 
  • #14
songoku said:
and due to east wind, the speed of the ambulance will be (50/3 - 5) cos 45 and the speed of the observer will be 5 cos 45 along AO?

thx
Let observer remain stationary and speed of ambulance remain unaffected by the wind.
You may get the equation as in your post #7
 
  • #15
Sorry i don't get why the speed of the sound along OB is 340 - 5 cos 45...

I think at B the wind still moves in the direction of the sound so it still adds up?

thx
 
  • #16
songoku said:
Sorry i don't get why the speed of the sound along OB is 340 - 5 cos 45...

I think at B the wind still moves in the direction of the sound so it still adds up?

thx
At B the sound is moving from B to O. The component of wind along the velocity is from O to B
 
  • #17
Oh i see

and for (c), we just neglect the wind?
 
  • #18
songoku said:
Oh i see

and for (c), we just neglect the wind?
No. It also adds up to the velocity of sound in both the directions.
 
  • #19
Oh i get it from the projection.

thx a lot rl.bhat ^^
thx also to turin and sam_goldberg ^^
 

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