The Simple Pendulum - Free Educational videos for Students in K-12 | Lumos Learning

The Simple Pendulum - Free Educational videos for Students in k-12


The Simple Pendulum - By The Organic Chemistry Tutor



Transcript
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 .
Summarizer

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.

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The Simple Pendulum is a free educational video by The Organic Chemistry Tutor.

This page not only allows students and teachers view The Simple Pendulum videos but also find engaging Sample Questions, Apps, Pins, Worksheets, Books related to the following topics.


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