The Simple Pendulum - By The Organic Chemistry Tutor
00:0-1 | in this video , we're going to talk about the | |
00:02 | simple pendulum . So let's begin by drawn our vertical | |
00:06 | life and let's dry pendulum . Let's put out an | |
00:12 | angle . Let's call this point A . B . | |
00:17 | And point C . Now as the pendulum moves from | |
00:24 | point A . To point B . And then the | |
00:26 | point C . And then as it returns from C | |
00:30 | . To A . That is one complete swing . | |
00:36 | Now the reason why I need to know what a | |
00:38 | complete swing is is because it can help you to | |
00:41 | determine the period and the frequency of a simple pendulum | |
00:47 | . The period represented by capital T . Is the | |
00:51 | time that it takes to make one complete swing that's | |
00:55 | going from A . To C . And then see | |
00:56 | to A . You can also calculate the period by | |
01:00 | , taken the time and divided by the number of | |
01:03 | cycles or the number of complete swings . So the | |
01:08 | period is measured in units of seconds . So it's | |
01:15 | the time that it takes to make one complete swing | |
01:18 | or one complete cycle . The frequency is the reciprocal | |
01:24 | of the period . To calculate the frequency , you | |
01:27 | could take the number of cycles or complete swings and | |
01:30 | divided by the time the unit of frequency is the | |
01:37 | reciprocal of the second . It's one of the seconds | |
01:40 | or equivalently hurts . Mhm . So make sure you | |
01:46 | understand that the period is the time it takes to | |
01:49 | make one complete cycle . Whereas the frequency is the | |
01:54 | number of cycles that occurs in 1/2 . Now , | |
01:57 | make sure that you're writing this down because you're going | |
01:59 | to use some of these formulas later when we work | |
02:02 | on something practice problems . Mhm . Now , in | |
02:05 | addition to the former is that we have on the | |
02:07 | board , there's some other formulas that you may want | |
02:10 | to add to your list . L . Is the | |
02:14 | left of the pendulum . Mhm . The period depends | |
02:19 | on the left of the pendulum . The period is | |
02:22 | equal to two pi times the square root of the | |
02:26 | left of the pendulum , divided by the gravitational acceleration | |
02:30 | . So G . Is the gravitational acceleration of the | |
02:32 | planet . So the gravitational acceleration for the Earth , | |
02:36 | as you know , it's 9.8 m/s squared . So | |
02:42 | the time it takes to make one complete swing depends | |
02:47 | on the left of the pendulum and the gravitational acceleration | |
02:51 | . As you can see , the mass is not | |
02:54 | part of that equation . Therefore the period of a | |
02:57 | simple pendulum is independent of the mass . If you | |
03:01 | increase the mass of the bob , it's not going | |
03:03 | to change the period of the pendulum . So when | |
03:07 | dealing with a simple pendulum , we're assuming that the | |
03:10 | mass of the string relative to the bob that it's | |
03:13 | attached to can be ignored . But for a typical | |
03:17 | test that you might take on this , just know | |
03:19 | that the period of a simple pendulum doesn't depend on | |
03:23 | the mass of the body . It only depends on | |
03:25 | these two things , the less than the gravitational acceleration | |
03:29 | . Now , since L . Is on top of | |
03:32 | that fraction increase in L . Will increase the period | |
03:39 | . That means that as you increase the length of | |
03:42 | the string , the time it takes for the bob | |
03:46 | to go from A . To C . And then | |
03:47 | see the A . And that time is going to | |
03:49 | increase . It's going to take longer to make the | |
03:53 | journey forward and then back . Now if you increase | |
03:57 | the gravitational acceleration , let's say if you brought the | |
04:00 | pendulum to a planet where the gravity is stronger , | |
04:05 | the period is going to decrease because she is in | |
04:09 | the denominator of that fraction . There's an inverse relationship | |
04:12 | between G . And T . Now To calculate the | |
04:20 | frequency , you could use this formula . The frequency | |
04:23 | is 1/2 pi times the square root of G over | |
04:27 | out . So since Ellis on the bottom as you | |
04:30 | increase l the frequency decreases . So the frequency the | |
04:37 | number of cycles that occur in one second where the | |
04:41 | number of complete swings that pendulum makes in a single | |
04:43 | second . That's inversely related to the left of this | |
04:49 | , the pendulum . But if you increase the gravitational | |
04:53 | acceleration , the frequency is going to go up . | |
04:59 | So if the period goes up the frequency goes down | |
05:03 | and if the period goes down the frequency goes up | |
05:07 | , so frequency and period they're inversely related . Now | |
05:11 | let's work on some practice problems . What is the | |
05:15 | period and frequency Of a simple pendulum ? That is | |
05:18 | 70 cm long . On the Earth and on the | |
05:21 | moon ? Yeah . So let's begin for picture . | |
05:28 | Mhm . So here is our pendulum . Yeah . | |
05:33 | And were given the length of the pendulum , it's | |
05:36 | 70 cm long . But we want to convert that | |
05:38 | to meters . So we know that 100 cm is | |
05:45 | equal to a meeting . So to convert from cm | |
05:49 | to m simply divide by a 100 and so the | |
05:52 | left is going to be point 70 m . What | |
06:00 | formula do we need in order to calculate the period | |
06:03 | and frequency in this problem ? To calculate the period | |
06:07 | . We could use this equation . It's two pi | |
06:10 | times the square root . Yeah of the left over | |
06:17 | the gravitational acceleration . Now on the Earth we know | |
06:20 | what the gravitational acceleration is . G . s 9.8 | |
06:27 | . It's not we just gotta plug in everything into | |
06:29 | this formula . So it's gonna be two pi times | |
06:31 | the square root of .7 m , divided by 9.8 | |
06:37 | m/s squared . So looking at the units the unit | |
06:42 | meters will cancel . And then when you take the | |
06:45 | square root of S squared is going to become S | |
06:49 | . Eventually . And so the period is going to | |
06:51 | be in seconds . Now let's go ahead and plug | |
06:55 | this in . So the period for part A or | |
07:06 | when the pendulum is on the earth , It's going | |
07:09 | to be 1.679 seconds . Now we need to calculate | |
07:15 | the frequency . The frequency is simply one over the | |
07:18 | period . So it's one divided by 1.67 , 9 | |
07:23 | seconds and you're going to get points 59 56 And | |
07:39 | then this is in , it's going to be second | |
07:41 | to the -1 or hurts . So that's the frequency | |
07:44 | for the first part . That is when the pendulum | |
07:47 | is on the Earth . Now let's move on to | |
07:50 | the next part . Yeah . So what about if | |
07:54 | the pendulum is on the moon ? What will be | |
07:59 | the period of the simple pendulum ? Now the gravitational | |
08:03 | acceleration on the moon is about 1.6 meters per second | |
08:08 | squared . So everything is gonna be the same except | |
08:12 | the value of G . Yes , So G is | |
08:20 | going to be 1.6 Instead of 9.8 . It's in | |
08:26 | the last problem . The period was I'm just going | |
08:31 | to write it here , It was 1.679 seconds . | |
08:37 | Yeah , that was on the Earth . Now , | |
08:40 | the period on the moon , let's call it . | |
08:42 | TM do you think it's going to be greater than | |
08:44 | 1.679 seconds or less than well as we go from | |
08:50 | the Earth to the moon ? The gravitational acceleration is | |
08:53 | decreasing . And since that's on the bottom of the | |
08:57 | fraction , it's inversely related to the period . That | |
09:01 | means when one goes up the other goes down or | |
09:03 | when one goes down the other goes up so G | |
09:06 | . Is decreasing . That means that the period is | |
09:08 | going to increase , so on the moon it's going | |
09:11 | to take a longer time to make a complete swing | |
09:15 | . So we should get an answer that's bigger than | |
09:17 | 1.679 seconds . So let's go ahead and plug this | |
09:21 | into our calculator . So this is going to be | |
09:30 | four 0.1 six seconds . Yeah . Yeah . So | |
09:41 | as you can see It's much bigger than 1.679 seconds | |
09:46 | . So as the gravitation of celebration decreases , the | |
09:48 | period is going to increase their inversely related . Now | |
09:52 | let's calculate the frequency . So the frequency is gonna | |
09:55 | be one over the period . So that's one over | |
09:58 | 4.16 seconds . And that's gonna be .24 Hz . | |
10:09 | So that's the frequency of the pendulum on the moon | |
10:13 | . Let's move on to our next problem . A | |
10:16 | Pendulum makes 42 cycles in 63 seconds . What is | |
10:20 | the period and frequency of the pendulum ? The period | |
10:28 | is going to be the time divided by the number | |
10:32 | of cycles . So we have 42 cycles occurring in | |
10:40 | the time period of 63 seconds . So if we | |
10:45 | take 63 divided by 42 or 63 seconds divided by | |
10:50 | 42 cycles , We get that there's 1.5 seconds per | |
10:55 | cycle . So the time that it takes to make | |
10:59 | one complete cycle is 1.5 seconds . So that we | |
11:02 | could say that the period Is 1.5 seconds . Yeah | |
11:09 | , so that's the answer for the first part of | |
11:11 | party . So now we can calculate the frequency , | |
11:14 | The frequency is one over the period . So it's | |
11:17 | one over 1.5 seconds . You're gonna get .6 repeat | |
11:26 | in which we profound that 2.67 . And you can | |
11:30 | say the units are second to the -1 hurts . | |
11:34 | So what this means is that There's .67 cycles that | |
11:40 | are occurring every second . So the units here , | |
11:45 | it's really technically one cycle divided by 1.5 seconds . | |
11:51 | And so you get points 67 cycles per second . | |
11:57 | So that's what the frequency in hertz is telling you | |
12:01 | , is the number of cycles that are occurring every | |
12:03 | one second Now . What about part B ? What | |
12:08 | is the length of the pendulum on Earth ? Okay | |
12:14 | , so let's clear away a few things and let's | |
12:17 | just rewrite . Mhm . The first two answers that | |
12:20 | we had . So how can we calculate the length | |
12:27 | of the pendulum when it's on the earth ? Well | |
12:31 | , let's start with this formats . He is equal | |
12:33 | to two pi times the square root of L . | |
12:37 | A V . G . We have the period and | |
12:40 | we know the gravitational acceleration of the Earth . We | |
12:43 | just need to isolate L . In this equation . | |
12:45 | So let's do some algebra . Let's square both sides | |
12:50 | of the equation . So on the left it's going | |
12:52 | to be t squared . two Pi squared is going | |
12:55 | to be two squared is four . And then pied | |
12:58 | some supplies , pi squared . And then when we | |
13:01 | square root , I mean when we take the square | |
13:03 | of a square root , both the square and the | |
13:06 | square , we will cancel . And so we're just | |
13:08 | going to get L O V E G . Mhm | |
13:13 | . Now we need to get all by itself . | |
13:16 | So we're going to multiply both sides by G . | |
13:18 | And then divide by four pi squared by doing this | |
13:25 | on the right side . We can cancel G . | |
13:27 | And we can also cancel four pi squared . So | |
13:31 | we're just going to get out on the right side | |
13:34 | . So we can say that L . Is equal | |
13:36 | to everything that we see here . So the less | |
13:39 | of the pendulum , it's going to be the gravitational | |
13:42 | acceleration G times the square of the period , divided | |
13:47 | by yeah , four pi squared . So that's the | |
13:51 | form of that . We can use to get the | |
13:52 | length of the pendulum . Now let's go ahead and | |
13:58 | plug everything in . Let's fight a unit as well | |
14:02 | . So G is going to be 9.8 meters per | |
14:05 | second squared . And then we're gonna multiply that by | |
14:09 | the square of the period . So that's 1.5 seconds | |
14:13 | squared . And then let's divide that by four pi | |
14:16 | squared , which doesn't contain units . So we can | |
14:20 | see that second squared will cancel with S squared here | |
14:24 | . And so L . Is going to be in | |
14:27 | meters . So let's plug in 9.8 times 1.5 squared | |
14:34 | divided by Now . You want to put this apprentices | |
14:36 | . Otherwise your calculated will divide by four and then | |
14:38 | multiply by pi square and you'll get a different answer | |
14:43 | . So let's divide by four pi squared in parentheses | |
14:46 | and you should get point 55 85 m . So | |
14:56 | this is the left of the pendulum on Earth that | |
14:59 | has these features . If you are transported to an | |
15:04 | unknown planet where the gravity of that planet is different | |
15:08 | from the earth , how can you determine the gravitational | |
15:13 | acceleration of that planet ? Well , this problem will | |
15:16 | help you to see how all you need is a | |
15:19 | simple pendulum . If you know the left of the | |
15:21 | pendulum and how many swings that the pendulum make in | |
15:25 | the given time period . You have all that you | |
15:28 | need to calculate or even estimate the gravitational acceleration of | |
15:33 | that planet . So let's work on this problem . | |
15:38 | The first thing we need to do is calculate the | |
15:39 | period , The period is going to be the time | |
15:45 | divided by the number of cycles . So this particular | |
15:53 | pendulum Makes 28 complete swings or 28 cycles in a | |
16:00 | time period Of 45 seconds . So let's divide 45 | |
16:05 | seconds by 28 cycles . And this will give us | |
16:09 | the period Which is 1.607 seconds per cycle . So | |
16:16 | this tells us that time it takes to complete one | |
16:19 | cycle . So it takes 1.607 seconds to make one | |
16:24 | complete swing . So that's the period now that we | |
16:28 | know the period . We could use this formula to | |
16:34 | calculate the gravitational acceleration , but we need to rearrange | |
16:38 | that formula . So like we did last time , | |
16:41 | let's go ahead and square both sides of this equation | |
16:45 | . So we're going to get T squared is equal | |
16:48 | to four pi squared , and the square root symbol | |
16:51 | will disappear . So it's gonna be times L over | |
16:54 | G . Now we need to get G by itself | |
17:00 | . So let's multiply both sides by G over T | |
17:04 | squared . So the left side , I'm going to | |
17:07 | multiply by G over T squared . Mhm . On | |
17:11 | the right side , G is going to cancel . | |
17:14 | On the left side , T squared is going to | |
17:15 | cancel . So the only thing that we have on | |
17:18 | the left side is G . So we have G | |
17:20 | is equal to four pi squared times L . And | |
17:26 | on the bottom we have T squared . So this | |
17:28 | is the form of that we could use to calculate | |
17:31 | the gravitational acceleration of any planet using a simple pendulum | |
17:36 | . All we need to know is the left of | |
17:38 | the pendulum , end of period or the time it | |
17:41 | takes to make one complete swing . So for this | |
17:45 | problem is going to be four pi squared times the | |
17:48 | left of the pendulum , which is 80 centimeters . | |
17:50 | Or if you divide that by 100 that's gonna be | |
17:53 | 1000.80 m And divided by the square of the period | |
17:58 | . The period is 1.607 seconds . Mhm . And | |
18:06 | don't forget to square . Yeah . So the answer | |
18:17 | is 12.2 meters per second squared . So this is | |
18:24 | the gravitational acceleration of the planet . Now , how | |
18:31 | many gs is this with respect to the Earth ? | |
18:36 | If we take that number and divided by the gravitational | |
18:40 | acceleration of the Earth ? Yeah , This is going | |
18:46 | to be 1.24 . So it's 1.24 Gs . So | |
18:51 | it's 1.24 times greater than the gravitational acceleration of the | |
18:55 | earth . So that's what that figure means whenever you | |
19:00 | see it , it simply compares the acceleration that you're | |
19:04 | experiencing with the acceleration of the Earth number four . | |
19:09 | What is the length of a simple pendulum used in | |
19:11 | a grandfather clock that has one second between its tick | |
19:15 | and it's talk on earth . So let's try a | |
19:18 | picture . Mhm . Feel free to pause the video | |
19:21 | and try this problem if you want to . So | |
19:25 | here is our simple pendulum . And let's label three | |
19:28 | points point a . B . And point C . | |
19:36 | Mhm . Actually get rid of that . So It's | |
19:40 | going to take 1 2nd for the grandfather clock to | |
19:43 | go from A . To C . Where it's going | |
19:45 | to make the first noise , it's tick noise . | |
19:49 | Then it's going to take another second for it to | |
19:51 | go from C . To A . Where it's going | |
19:53 | to make the talk noise . So it's like tic | |
19:55 | tac tic tac and just oscillates between A . And | |
19:59 | C . So we need to realize is that The | |
20:02 | period is not 1 2nd , but two seconds . | |
20:06 | It takes two seconds to make a complete swing . | |
20:09 | The 1 2nd is just , it's half of a | |
20:13 | cycle . It's going from A to C . But | |
20:15 | doesn't include the return trip . So the period for | |
20:19 | grandfather clock is two seconds . So with that information | |
20:23 | , we can now calculate the length of the simple | |
20:26 | pendulum that is in their grandfather clock . And so | |
20:31 | we're going to use this formula L . Is equal | |
20:33 | to GT squared divided by four pi squared . Yeah | |
20:41 | . Mhm . So on Earth G . is 9.8 | |
20:45 | . The period for the grandfather clock is two seconds | |
20:49 | and then divided by four pi squared . And let's | |
20:52 | put that in parentheses as well . And I almost | |
21:05 | forgot to square the period . So don't make that | |
21:08 | mistake . So the answer is going to be point | |
21:16 | 993 m . So that that's the length of the | |
21:20 | grandfather clock . Given a period of two seconds , | |
21:24 | number five , A certain pendulum has a period of | |
21:28 | 1.7 seconds on Earth . What is the period of | |
21:32 | this pendulum on a planet that has a gravitational acceleration | |
21:36 | of 15 m/s squared ? Well , in order to | |
21:41 | calculate the period , we can use this formula , | |
21:44 | it's two pi times the square root of L over | |
21:47 | G . But let's write down what we know in | |
21:50 | this problem and what we need to find . So | |
21:53 | the period on the earth , let's call it t | |
21:55 | . one . That's 1.7 seconds . Now we know | |
22:00 | that the gravitational acceleration on the Earth , We'll call | |
22:03 | that G . one is 9.8 meters per second squared | |
22:08 | . We wish to calculate the new period on some | |
22:11 | other planet T . Two and were given the gravitational | |
22:15 | acceleration Of that planet , which is 15 m/s squared | |
22:20 | . So we have T . One N . G | |
22:22 | one . How can we calculate T . Two if | |
22:24 | we know G . Two . Well let's make a | |
22:28 | ratio of this equation . We're going to divide teach | |
22:31 | you by T . one . So if T . | |
22:34 | Is equal to what we see here T . two | |
22:37 | is going to be two pi square root L over | |
22:42 | G . Two . Now the reason why I didn't | |
22:45 | write L . Two of G two is because L | |
22:47 | . Doesn't change . We're dealing with the same pendulum | |
22:51 | that was on the earth that is now in this | |
22:53 | new planet . So therefore Ellis constant . We don't | |
22:56 | need to change the sub script for al only GMT | |
23:00 | changes . So it's the one it's going to be | |
23:06 | two pi times the square root of L . Over | |
23:09 | G . Mark . Mhm . So we can cross | |
23:12 | out to pie and we can cancel out . Yeah | |
23:17 | . and so we're left with T . two over | |
23:19 | T one is equal to The square root of one | |
23:23 | over G two Divided by the square root of one | |
23:26 | over G . One . Now let's multiply the top | |
23:30 | and the bottom by the square root of G . | |
23:32 | one . Doing so well give us someone in the | |
23:40 | denominator . So it's going to be The square root | |
23:44 | of this is one times G one . So we'll | |
23:48 | have G1 on the top . G two is going | |
23:50 | to stay in the bottom And then this simply becomes | |
23:54 | one . The square root of one is 1 . | |
23:57 | So we could say that T two over T one | |
24:00 | is equal to the square root of G . One | |
24:02 | over G . Two . And then finally we can | |
24:07 | multiply both sides by T . one to cancel this | |
24:13 | . So we have this equation . The second period | |
24:17 | T two is going to equal the first period Times | |
24:20 | The Square Root of G . one Over G two | |
24:24 | . Yeah . Now let's plug in some values . | |
24:30 | T one is 1.7 . G one is 9.8 . | |
24:35 | G two is 15 So 1.7 times the square root | |
24:43 | of 9.8 over 15 , That's going to be 1.37 | |
24:50 | seconds . So that's the new period . So as | |
24:56 | we could see , we increase the gravitational acceleration from | |
25:01 | 9.8-15 and because Gs on the bottom , it's inversely | |
25:05 | related to T . So as we increase G The | |
25:09 | period decreased , it went from 1.7 To 1.37 seconds | |
25:15 | . So these two are inversely related Number six . | |
25:20 | The period of a simple pendulum with mass m . | |
25:23 | s.t . Which of the following expressions represent the period | |
25:27 | of a simple pendulum with mass to em . Well | |
25:33 | , if we write the formula for the simple pendulum | |
25:37 | , notice that it doesn't depend on a mass , | |
25:40 | so if we change the mass from EM 22 M | |
25:44 | , it's not going to change your period . The | |
25:46 | period was initially t it's going to remain team . | |
25:50 | So for a simple pendulum , the period is independent | |
25:55 | from the mass . It doesn't change with the mass | |
25:59 | , so the answer is going to be deep . | |
26:00 | There's no change . |
DESCRIPTION:
This physics video tutorial discusses the simple harmonic motion of a pendulum. It provides the equations that you need to calculate the period, frequency, and length of a pendulum on Earth, the Moon, or another planet. This video contains plenty of examples and practice problems.
OVERVIEW:
The Simple Pendulum is a free educational video by The Organic Chemistry Tutor.
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