How To Solve Doppler Effect Physics Problems - By The Organic Chemistry Tutor
00:00 | in this video , we're going to talk about the | |
00:02 | Doppler effect . The Doppler effect is a phenomenon where | |
00:07 | the frequency that is detected by some observer changes because | |
00:13 | either the source is moving or the observer is moving | |
00:18 | . So let's say we have a source and this | |
00:23 | source emits sound waves in all directions . Mhm . | |
00:29 | And let's say we have an observer . If the | |
00:37 | source moves towards the observer or if the observer moves | |
00:43 | towards the source of the sound waves , the frequency | |
00:48 | that is detected by the observer , that's awful . | |
00:51 | That frequency is going to increase . Which means the | |
00:55 | frequency measured by the observer will be greater than the | |
00:58 | frequency of the source . So let me give an | |
01:04 | example of some numbers . So let's say you have | |
01:07 | a source that's moving towards this person . The source | |
01:14 | may have a frequency of 800 hertz , but the | |
01:18 | frequency that the person will here is going to be | |
01:21 | higher than 100 It might be 8:50 Hz . And | |
01:27 | so that's the basic idea behind the Doppler effect . | |
01:30 | When either the source or the observer is moving , | |
01:34 | the detective frequency is going to shift is gonna be | |
01:36 | different than the original frequency that the source emitted . | |
01:42 | So whenever the source or the observer move towards each | |
01:46 | other , the observed frequency is going to be bigger | |
01:49 | than the source frequency . Now the reverse is true | |
01:53 | . Let's say if the source is moving away from | |
01:57 | the observer or if the observer is moving away from | |
02:01 | the source , then the frequency that the observer to | |
02:06 | text that's going to decrease , which means that it's | |
02:10 | going to be less than the original frequency emanated or | |
02:13 | emitted by the source . Now let's try a picture | |
02:18 | . So here's a source and we're going to draw | |
02:22 | some waves around the source . Okay , my drawing | |
02:32 | is not perfect , but we'll make the best of | |
02:34 | that . Let's make one more wave . So let's | |
02:45 | say we have a person here , we'll say this | |
02:48 | is john and to the left is Karen . Now | |
03:00 | the source of the sound wave , this could be | |
03:02 | like an ambulance trunk or a police car . This | |
03:07 | is moving towards john . And let's say that the | |
03:10 | frequency emitted by the source is 1000 Hz , john | |
03:20 | let's say john and Karen are stationary observers . They're | |
03:23 | not moving . So their speed , their video is | |
03:27 | zero . Now , as the source of the sound | |
03:33 | moves towards john , the frequency that john is going | |
03:36 | to hear , it's going to be higher Than 1000 | |
03:39 | . It might be 1100 . Now the source is | |
03:43 | moving away from Karen . So the frequency that Karen | |
03:47 | detects , It's going to be less than 1000 . | |
03:50 | It's gonna be like maybe 900 or 800 . And | |
03:55 | let's talk about why , as the source moves toward | |
03:59 | john notice that the distance between the crests of the | |
04:04 | waves is decreasing . So therefore the wave left is | |
04:07 | decreasing . Whenever the wavelength decreases the frequency increases . | |
04:13 | So that's one of the reasons why the frequency increases | |
04:17 | as the source moves towards john is because the distance | |
04:21 | between waves is decreasing . But now as the source | |
04:28 | moves away from Karen , we can see that the | |
04:30 | distance between the waves is increasing . So as the | |
04:35 | wavelength goes up , the frequency goes down . Mhm | |
04:40 | . So any time the source moves away from a | |
04:43 | person , the frequency is going to go down because | |
04:45 | the wavelength is increasing when the source moves towards a | |
04:48 | person , the wavelength decreases . And so the frequency | |
04:52 | goes up . So that's a visual representation of how | |
04:56 | the Doppler effect work when the source is moving and | |
04:59 | the observer's stationary . But now let's talk about the | |
05:02 | formula that we could use to solve problems . The | |
05:07 | observed frequency is equal to the frequency of the source | |
05:13 | , times V . And then it's plus or minus | |
05:20 | . Vienna over V . And then you can write | |
05:24 | this as plus or minus or minus plus . You | |
05:29 | can still get the right answer , regardless of how | |
05:30 | you choose to write to write the equation . What | |
05:34 | you need to realize is that V is the speed | |
05:36 | of sound , Which is 343 m/s . Now the | |
05:41 | speed of sound in air is dependent on the temperature | |
05:45 | . And here's the formula that describes that relationship . | |
05:48 | The speed of sound is approximately 331 plus .60 . | |
05:56 | Where T . Is the temperature in Celsius , and | |
05:59 | V is going to be the speed in meters per | |
06:00 | second . So at a temperature of 0°C, , this | |
06:06 | disappears to simply get a speed of Approximately 331 meters | |
06:14 | for a second . When the temperature is 20°C, , | |
06:18 | based on that equation , the speed is let me | |
06:21 | use the approximate symbol . It's approximately 343 m for | |
06:25 | a second And at 25°C, , the speed is approximately | |
06:33 | 346 m/s , So the speed increases by .6 m/s | |
06:40 | for every increase in 1°C in temperature . When the | |
06:44 | temperature increases by 5°C, , the speed Increases approximately by | |
06:50 | three m/s . So that's the formula . That would | |
06:53 | help you to get an estimate of the speed of | |
06:55 | sound in air given the temperature . But if the | |
06:59 | temperature is not specified , We're going to assume that | |
07:03 | the temperatures at 20°C. . So we're gonna go with | |
07:05 | this number . So if you're not giving the temperature | |
07:08 | or the speed of sound , simply use 343 m/s | |
07:12 | for the problems that we're going to solve in this | |
07:14 | video . Yeah . Now in order to use this | |
07:18 | equation successfully , you need to know when to use | |
07:22 | the positive sign and the negative sign in the numerator | |
07:25 | and the denominator of that fraction . So how do | |
07:30 | we choose when to use what sign ? Mhm . | |
07:34 | Well , we need to have understanding of fractions . | |
07:38 | A fraction is made up of two parts . There | |
07:42 | is the new murder on the top and the denominator | |
07:46 | on the bottom . Now what you need to know | |
07:49 | is that the value of the numerator is proportional to | |
07:53 | the value of the fraction . So what does that | |
07:54 | mean when you increase the value of the numerator ? | |
07:57 | The value of the fraction goes up . So in | |
08:00 | that sense the proportional , what happens to one happens | |
08:03 | to the other . If you decrease the value of | |
08:06 | the numerator , the value of the fraction goes down | |
08:11 | . Now the situation is different for the denominator of | |
08:13 | a fraction . Yeah the denominator is inversely related to | |
08:19 | the value of the entire fraction . That means one | |
08:22 | goes up , the other goes down . So if | |
08:23 | you were to increase the value of the denominator the | |
08:28 | value of the entire fraction decreases . And if you | |
08:30 | decrease the value of the denominator the value of the | |
08:33 | entire fraction increases . So make sure you understand that | |
08:36 | relationship . Feel free to write this down because we're | |
08:40 | going to use it to talk about when to use | |
08:42 | these sides . So let's consider the first situation that | |
08:50 | is when the source is moving towards the observer . | |
09:00 | So V . S . Represents the speed of the | |
09:04 | source . Vo represents the speed of the observer . | |
09:11 | If the observer is stationary that means video is zero | |
09:15 | . If the source is stationary that means v . | |
09:16 | s . zero . But let's say in a situation | |
09:19 | the observer's stationary but the source is moving towards the | |
09:22 | observer . What sign should we use in front of | |
09:26 | the S . Should it be positive or negative ? | |
09:30 | So the fact that the source is moving towards the | |
09:32 | observer , what's going to happen to the frequency that | |
09:35 | is fo anytime one moves towards the other , do | |
09:39 | we know the frequency is going to be higher , | |
09:41 | S . O . Is going to increase . Now | |
09:50 | V . S . Is in the denominator of the | |
09:52 | fraction . So if we want the whole fraction to | |
09:56 | increase , should we increase the denominator or should we | |
10:00 | decrease it ? Well we know the denominator is inversely | |
10:04 | related to the value of fraction . So if we | |
10:07 | want the value of the entire fraction to go up | |
10:11 | we need the denominated to go down . So therefore | |
10:14 | the only way we can decrease the value of the | |
10:17 | denominator is to use a negative in front of us | |
10:21 | . So when a source moves towards the observer we're | |
10:24 | going to use negative V . S . That's going | |
10:28 | to decrease the value of the denominator which will increase | |
10:31 | the value of the fraction . And so the observed | |
10:34 | frequency is going to be higher than the source frequency | |
10:40 | . Now let's consider the other situation that is when | |
10:45 | a source moves away from the observer . When the | |
10:51 | source moves away from the observer , we know that | |
10:53 | the frequency that is observed or detected by the observer | |
10:57 | that has to go down the source velocity is still | |
11:00 | in the bottom of the fraction , it's still in | |
11:02 | the denominator . So the only way we can decrease | |
11:06 | the value of the entire fraction to get it lower | |
11:09 | fo value is to increase the value of the denominator | |
11:13 | . So we need to use positive V . S | |
11:18 | . If we increase the value of the denominator the | |
11:20 | value the whole fraction goes down fo becomes less than | |
11:23 | Fs . Now let's consider the next situation . Mhm | |
11:32 | . So here we have the source and this time | |
11:36 | the observer is going to move toward the source . | |
11:43 | Now when the observer moves towards the source we know | |
11:45 | that the detective frequency is going to increase and we're | |
11:49 | dealing with video . No nevius and video is in | |
11:51 | the numerator of the fraction . So should we use | |
11:57 | positively or negatively ? Oh what would you say ? | |
12:01 | Well since F . O . Is going to increase | |
12:03 | the value of the entire fraction has to go up | |
12:06 | and to accomplish that using the numerator we need the | |
12:08 | numerator to increase . So therefore we need to use | |
12:11 | a positive sign for video that's going to increase the | |
12:14 | numerator . Now what about if the observer is moving | |
12:23 | away from the source ? If he's moving away F | |
12:29 | . O . Is going to decrease . So in | |
12:31 | order to decrease the value of the whole fraction we | |
12:34 | need to decrease the numerator . So therefore we need | |
12:36 | to use a negative sign in front of vo . | |
12:41 | So let's put this all together in one page . | |
12:43 | And what I'm gonna do is I'm going to reverse | |
12:45 | the position of the source and the observer because the | |
12:48 | signs of V . Will correspond to the direction of | |
12:51 | the arrow along the X . Axis . So in | |
13:01 | this situation we're going to have the source moving towards | |
13:06 | the observer . And when that happens we're going to | |
13:11 | use negative V . S . Notice that the arrow | |
13:14 | is pointing towards the left . If you put the | |
13:16 | source on the right and the observer on the left | |
13:19 | , the direction of the arrow is going to correspond | |
13:21 | to the sign in front of the , So when | |
13:23 | the source moves towards the person who's negative , yes | |
13:27 | the denominator will decrease and the value of the fraction | |
13:30 | . And does the detective frequency will go up Now | |
13:34 | for the next scenario . Mhm . The source is | |
13:44 | moving away from the observer . So we're gonna use | |
13:51 | positive V . S . Notice that the arrow it's | |
13:58 | pointing towards the right in the positive X . Direction | |
14:03 | . So in this case the denominator is going to | |
14:05 | increase in value . The frequency is gonna decrease in | |
14:09 | value . Now for the next situation here's the observer | |
14:18 | and this time the observer is going to move towards | |
14:21 | the source . As the observer moves towards the source | |
14:28 | , we know that the detective frequency is gonna go | |
14:30 | up . And so the numerator has to go up | |
14:34 | . And thus we need to use positive Vo Now | |
14:43 | for the 4th situation the observer is moving away from | |
14:47 | the source . so the detective frequency is going to | |
14:54 | go down and the numerator must go down in order | |
14:56 | to accomplish that . So this is going to be | |
14:59 | negative vo . So as you can see when you | |
15:04 | place the observer on the left and the source on | |
15:06 | the right , the sign in front of the corresponds | |
15:10 | to the direction of the arrow . So it's negative | |
15:12 | going towards the left , positive , going towards the | |
15:15 | right . If we put the observer on the left | |
15:17 | and the source on the right , That's only one | |
15:20 | . It's gonna work out that way . But any | |
15:22 | time the source or the observer Moves toward one another | |
15:30 | . In all cases , we see that the observed | |
15:34 | frequency increases and whenever either the source or the observer | |
15:42 | moves away from each other , the detective frequency decreases | |
15:49 | . So make sure you understand the concept of the | |
15:50 | Doppler effect . So now let's work on some problems | |
15:56 | . Number one , An ambulance truck emits a sound | |
16:00 | with a frequency of 800 Hz part A what is | |
16:04 | the frequency detected by a stationary observer ? If the | |
16:08 | ambulance truck is moving 30 m/s toward the observer And | |
16:13 | were given the speed of sound and air at 20°C, | |
16:15 | , which is 343 m/s . So let's go ahead | |
16:21 | and work on this problem . Let's draw a picture | |
16:23 | . Now , it's going to make it a lot | |
16:24 | easier if we put the observer on the less and | |
16:29 | we're going to put the source on the right , | |
16:35 | the source is going to be the ambulance truck . | |
16:38 | It's admitting a sound With the frequency of 800 Hz | |
16:44 | . The frequency is also related to the pitch . | |
16:47 | They're the same . So a sound with a high | |
16:50 | pitch has a high frequency . Now this ambulance truck | |
16:55 | , which is the source , it's moving towards the | |
16:58 | Observer . And here's the formula fo is equal to | |
17:05 | F . S . And then it's V . Plus | |
17:08 | or minus V . S . I mean that should | |
17:12 | be vo over the V . Plus or minus V | |
17:15 | . S . Mhm . So we need to determine | |
17:19 | if the S . Should be positive or negative . | |
17:22 | So the arrow points towards the left V . S | |
17:25 | . Is going to be negative . So if we | |
17:30 | choose a negative value we know that the denominator is | |
17:35 | going to decrease and the value of the whole fraction | |
17:38 | and thus fo is going to increase . Which is | |
17:41 | what should happen whenever the source moves towards the Observer | |
17:45 | . The detective frequency should go up . So now | |
17:49 | that we know which time we need to use , | |
17:51 | we can go ahead and get the answer . So | |
17:54 | the source frequency is 800 . The speed of sound | |
17:58 | is 343 . The observer is stationary so he's not | |
18:04 | moving anywhere . Vo is zero and then V . | |
18:10 | S . We're going to use a negative value . | |
18:13 | The source is moving towards the observer at 30 m/s | |
18:18 | . So this is going to be 800 Times 3 | |
18:21 | 43 and then 3 43 -30 . That's 3 13 | |
18:34 | . So the detective frequency measured by the observer Is | |
18:38 | approximately 877 Hz . So this is the answer to | |
18:46 | part A . Now let's move on to part B | |
19:00 | . What frequency will be detected if the ambulance truck | |
19:03 | is moving 30m/s away from the observer . So we | |
19:10 | still want the source to be to the right of | |
19:11 | the observer . And let's rewrite the equation . Mhm | |
19:30 | . Now what should we use for the sign of | |
19:31 | the S . So the arrow is pointing towards the | |
19:34 | right , This is going to be positive V . | |
19:37 | S . So this works if you put the observer | |
19:42 | on the left and the source on the right . | |
19:46 | Now as we could see when if we choose a | |
19:48 | positive sign for V . S . The denominator will | |
19:51 | increase in value . And so the value of the | |
19:54 | whole fraction is going to go down and the source | |
19:56 | as it moves away from the observer , we expect | |
20:00 | that the detective frequency or the observed frequency should be | |
20:03 | less than the original source frequency . So let's go | |
20:09 | ahead and get the answer . The source frequency is | |
20:11 | still 800 . The speed of sound is still 343 | |
20:19 | . Vo is still zero . But this time we're | |
20:21 | going to use positive V . S . And v | |
20:24 | . s . is 30 . So it's going to | |
20:27 | be 800 Times 3 43 And then 3 43 plus | |
20:32 | 30 . That's 373 . Mhm . So this is | |
20:43 | going to be 700 And 36 Hz . So as | |
20:50 | you can see it's less than 800 , which is | |
20:53 | what should happen when the source moves away from the | |
20:57 | observer , the pitch or the frequency should decrease . | |
21:02 | So that's how you can solve some basic Doppler effect | |
21:05 | problems in physics . Number two , A stationary ambulance | |
21:10 | truck emits a frequency of 1200 hertz , calculate the | |
21:14 | frequency detected by the observer if the observer is driving | |
21:19 | toward the ambulance truck At 25 m/s . So , | |
21:25 | let's begin with a picture . We're going to put | |
21:27 | the observer on the left side just like before . | |
21:31 | And we're gonna put this source on the right side | |
21:34 | . Mm hmm . Yeah . Now this problem , | |
21:41 | the observer is moving towards the source . Mhm . | |
21:47 | Now , let's write our formula . Yes . Mhm | |
21:55 | . Yeah . So we need to determine if we're | |
21:57 | going to use positive or negative . Yes vo yeah | |
22:03 | . Mhm . So what would you say should it | |
22:07 | be plus video or minus field ? Well because the | |
22:11 | observer is moving towards the source and for this particular | |
22:15 | situation it's gonna be plus video . And here's how | |
22:22 | we can reason . Like we've been reasoning before as | |
22:27 | the observer moves towards the source , we know that | |
22:30 | the detective frequency has to go up and since the | |
22:33 | video is in the numerator , the only way in | |
22:36 | which we can increase the detective frequency using the numerator | |
22:40 | is to increase the numerator . And that can only | |
22:43 | happen if we use positive field . So now that | |
22:50 | we know the sign of the oh we can plug | |
22:52 | in the data that we have . So the source | |
22:56 | frequency is 1200 V . And this problem is 343 | |
23:06 | , The sources stationary Soviet zero and then video Is | |
23:12 | moving at 25 minutes per second . So that's the | |
23:15 | observer Now 3 43 plus 25 . That's going to | |
23:24 | be 368 . And we're gonna divide that by 343 | |
23:36 | . So for part A the frequency measured by the | |
23:40 | Observer , It's going to be 1200 87.46 . But | |
23:47 | let's find that 10 nearest whole number . So we'll | |
23:49 | say 1287 Hz . Mhm . So that's the frequency | |
23:54 | that the driver is going to detect as he moves | |
23:58 | towards the ambulance truck . Mhm . Now let's move | |
24:04 | on to Part B . Yeah . In part B | |
24:12 | . The observer is driving away from the ambulance truck | |
24:16 | . So this time he's going in this direction . | |
24:20 | So it's going to be negative V . S . | |
24:26 | Because he's moving away . We know that the detective | |
24:30 | frequency will decrease relative to the source frequency . And | |
24:35 | to accomplish that we need to decrease the numerator . | |
24:38 | So we need to use I put the sm into | |
24:41 | put Vo so we need to use a negative vo | |
24:47 | . Yeah so let's go ahead and plug that in | |
24:53 | . So the source frequency is still 1200 Via still | |
24:58 | 3 43 . The S . Is still zero . | |
25:02 | But the only thing that's different here is we're gonna | |
25:04 | plug in negative video which is So it's gonna be | |
25:09 | negative 25 3 43 -25 is 3 18 . So | |
25:25 | it's gonna be 1200 times 318 divided by 343 . | |
25:30 | And so for part B . The frequency picked up | |
25:33 | by the observer . It's going to be if you | |
25:35 | run into nurse hole number 1113 Hz . Mhm . | |
25:41 | Mhm . So as you can see it's less than | |
25:44 | 1200 because the driver is moving away . But for | |
25:48 | the first part it's greater than 1200 because the driver | |
25:51 | is moving towards the source of the sound . Now | |
25:57 | let's move on to the next problem . # three | |
26:00 | . A police car is moving west at 20 m/s | |
26:04 | Toward a driver who is moving east at 25 m/s | |
26:09 | . The police car emits a frequency of 900 Hz | |
26:13 | . What frequency is detected by the driver . So | |
26:18 | feel free to try this problem for the sake of | |
26:20 | practice . Now , let's try a picture . So | |
26:25 | as long as we place the observer on the left | |
26:27 | side and the source on the right side , the | |
26:32 | science of VO NVs , they're going to match with | |
26:38 | the direction of the velocity of these two objects along | |
26:43 | the X axis . Now , the police car , | |
26:50 | which is basically the source of the sound , it's | |
26:54 | going to be moving west , so it's going this | |
26:58 | way At a speed of 20 m/s . Yeah , | |
27:07 | now the driver Is moving east or towards the right | |
27:10 | at a speed of 25 m/s . So automatically because | |
27:15 | we have the observer on the left and a source | |
27:17 | in the right , the direction of the arrow is | |
27:19 | going to be the same as it's going to be | |
27:22 | aligned with the sign of V . O . And | |
27:24 | V . S . So we're gonna use a positive | |
27:28 | value for Vo and a negative value for V . | |
27:32 | S . And just to confirm it , the observer | |
27:38 | is moving towards the source so that action will increase | |
27:42 | the detective frequency . Video is in the numerator . | |
27:46 | The fraction . So in order to increase the frequency | |
27:50 | needs to increase the value of the new mirror . | |
27:52 | And so we need to choose a positive value for | |
27:54 | video as opposed to a negative value . Now the | |
27:58 | action taken by the source as it moves towards the | |
28:01 | observer . That action will also increase the detective frequency | |
28:06 | . V . S . Is in the denominator of | |
28:09 | the formula . And in order to increase the value | |
28:12 | of the fraction we need to decrease the value of | |
28:15 | the denominator . And we can accomplish that by using | |
28:18 | negative Gs . So I want you to understand how | |
28:22 | that works because that can help you to choose the | |
28:26 | appropriate sign if these two are not in the the | |
28:31 | right position . So now that we have everything that | |
28:36 | we need , let's go ahead and plug it in | |
28:40 | two our floor line . Mhm . Yeah so the | |
28:54 | observed frequency is going to equal the source frequency which | |
28:58 | in this problem That's 900 Hz . And then that's | |
29:06 | gonna be 3 43 . Now we're gonna use plus | |
29:10 | vo so the speed of the observer Is 25 m/s | |
29:20 | . And then we're going to use -3 . The | |
29:25 | speed of the source or the police car is moving | |
29:27 | 20 m/s west . So this is going to be | |
29:32 | 900 3 43 plus 25 . We know that's 368 | |
29:40 | . 3 43 -20 . That's 3 23 . So | |
29:47 | 900 times 3 68 divided by 3 23 . So | |
29:53 | we get this answer , The observed frequency , it's | |
29:55 | going to be 1000 25 hertz . So as we | |
30:01 | can see it's significantly higher then The source frequency of | |
30:06 | 900 because both the source and the observer are moving | |
30:12 | toward each other , so that's going to greatly increase | |
30:15 | the frequency that is detected by the Observer . |
DESCRIPTION:
This physics video tutorial provides a basic introduction into the doppler effect of moving sound waves. it explains how to solve doppler effect problems in physics. Any time the source moves toward the observer or if the observer moves toward the source, the detected frequency will increase - that is - the observed frequency will be greater than the frequency emitted by the source. The source can be an ambulance truck or a police siren. If the source moves away from the observer or if the observer moves away from the source, the detected frequency will decrease. This video contains plenty of examples and practice problems of calculated the frequency detected by the observer.
OVERVIEW:
How To Solve Doppler Effect Physics Problems is a free educational video by The Organic Chemistry Tutor.
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