Conservation of Energy Physics Problems - By The Organic Chemistry Tutor
Transcript
00:01 | Let's work on this problem . A block slides down | |
00:04 | a 150 m inclined plane , as shown in the | |
00:07 | picture below , starting from us , what is the | |
00:10 | speed of the block when it reaches the bottom of | |
00:13 | the incline ? So we're gonna use conservation of energy | |
00:17 | to solve this problem . So the initial mechanical energy | |
00:23 | has to equal the final mechanical energy . The only | |
00:27 | forces acting on the block , Our conservative forces like | |
00:32 | gravity . So mechanical energy is can serve at point | |
00:37 | A . The only form of energy that we have | |
00:39 | is potential energy . And that point B . Choosing | |
00:43 | this as the ground level , there's no potential energy | |
00:45 | A point B . However , the block will have | |
00:48 | kinetic energy at point B . So we can set | |
00:51 | these two equal to each other As the block slides | |
00:54 | down , potential energy is being converted to kinetic energy | |
00:59 | . The potential energy of the block is MGH and | |
01:02 | the kinetic energy of the block is one half mv | |
01:05 | squared so we could cancel them . Therefore we don't | |
01:09 | need to master block . Now , I'm going to | |
01:12 | multiply both sides by two , so on the left | |
01:15 | have to G . H . Is equal to two | |
01:18 | times a half these will cancel . So that's one | |
01:21 | and that's going to equal the square , taking the | |
01:24 | square root of both sides . The final speed is | |
01:27 | going to be the square root of two G . | |
01:29 | H . So let's go ahead and plug everything that | |
01:34 | we have . So it's two times the gravitational acceleration | |
01:39 | of 9.8 Time is the height of the block , | |
01:42 | which is 150 m high . So by the way | |
01:46 | , this is the height , So that's 150 m | |
01:52 | . So if you type this in your calculator , | |
01:58 | you should get 54 0.22 m/s . So without friction | |
02:06 | , that's how fast this block is going to be | |
02:08 | moving when it features position be number two . An | |
02:15 | eight kg Block compresses a horizontal spring By 2.5 m | |
02:20 | beyond its natural length . As shown in the figure | |
02:23 | below , what is the speed of the block ? | |
02:26 | As soon as it's released from the spring ? So | |
02:29 | let's call this position A an opposition B when it's | |
02:32 | still on level ground , you want to find the | |
02:35 | speed as soon as it's release . So opposition eh | |
02:41 | The block spring system has potential energy . Elastic potential | |
02:45 | energy energy is stored in the spring and what's its | |
02:50 | release ? That energy is going to be converted to | |
02:52 | kinetic energy . Now the height doesn't change . So | |
02:56 | there's no gravitational potential energy . So we can say | |
03:00 | the elastic potential energy will be equal to the kinetic | |
03:03 | energy of the block . Energy is going to be | |
03:06 | transferred from the spring to the block . The elastic | |
03:10 | potential energy is 1/2 KX Square . The kinetic energy | |
03:14 | is 1/2 M . V . Squared . If we | |
03:17 | multiply both sides by two , we can get rid | |
03:19 | of the fraction . So now we're going to start | |
03:23 | for the speed . So we have K . Which | |
03:26 | is 300 And X . is the amount the spring | |
03:30 | is compressed by which is 2.5 m . The mass | |
03:34 | of the block is eight . To let's calculate the | |
03:36 | final speed 300 times 2.5 Squared is 1875 . And | |
03:43 | if we divide that by eight , That's going to | |
03:46 | be 234.375 . And that's equal to V squared . | |
03:53 | Now let's take the square root of both sides . | |
04:00 | So the speed is going to be 15.31 meters per | |
04:05 | second . So this is the answer to part eight | |
04:10 | . That's gonna be the speed of the block as | |
04:14 | soon as it's released opposition B now part B . | |
04:18 | How high up the hill with a black . Oh | |
04:21 | so let's see if it gets up to that height | |
04:23 | . How can we calculate H . Now ? Opposition | |
04:27 | be the block has kinetic energy opposition . See where | |
04:31 | it comes to rest . It's no longer going to | |
04:33 | have any kinetic energy . The only energy is going | |
04:36 | to have is gravitational potential energy . Mhm . So | |
04:41 | what we need to do is that the kinetic energy | |
04:46 | equal to the gravitational potential energy . So this is | |
04:49 | gonna be one half Mv squared and that's going to | |
04:52 | equal M . G . H . So once again | |
04:55 | we could cancel em . Now let's go ahead and | |
04:59 | plug in everything that we have . So it's one | |
05:01 | half times v . Squared which is 15.31 square and | |
05:06 | that's equal to G . Times H . So 15.31 | |
05:13 | Squared times 0.5 Divided by 9.8 will give us a | |
05:20 | height of about 12 m if you wanted to nurse | |
05:24 | whole number . So that's how high the block is | |
05:29 | going to go before it comes to rest . Number | |
05:33 | three , A 10 kg Block slides down a hill | |
05:38 | That is 200 m tall . As shown in the | |
05:41 | figure below With an initial speed of 12 m/s . | |
05:47 | What is the speed of the block when it reaches | |
05:49 | the bottom of the hill ? At let's say position | |
05:52 | be assuming there's no friction . So opposition . A | |
06:01 | Let's call that the original position . The block has | |
06:05 | potential energy because it's above position be . It has | |
06:11 | the capability of falling now because the block is in | |
06:14 | motion . It has kinetic energy . Opposition being It's | |
06:19 | only going to have kinetic energy so opposition A . | |
06:25 | We have potential energy and kinetic energy . Opposition be | |
06:31 | We only have kinetic energy . So all of the | |
06:34 | potential energy opposition came is going to go to the | |
06:38 | kinetic energy of the object . The object speed will | |
06:41 | increase beyond 12 m/s . So let's go ahead and | |
06:45 | calculate that speed . So this is going to be | |
06:48 | MGH plus one half and the initial square . So | |
06:54 | the initial speed is 12 . We're looking for the | |
06:56 | final speed And that's equal to the final kinetic energy | |
06:59 | of 1/2 MV Final Square . So we could divide | |
07:04 | everything by em and multiply everything by two . So | |
07:08 | it's gonna be to G . H . Plus the | |
07:12 | initial squared and that's equal to the final square . | |
07:15 | So basically that looks like this equation . The final | |
07:18 | squared is equal to the initial squared plus two A | |
07:21 | . D . That's a formula that you've seen in | |
07:24 | schematics . So let's calculate the final speed . So | |
07:31 | the final squared is equal to the initial squared which | |
07:33 | is 12 square plus two times the gravitational acceleration Times | |
07:39 | A height of 200 . So it's 12 square plus | |
07:45 | two times 9.8 times 200 . And that's 4064 and | |
07:50 | then take the square root of that number . And | |
07:53 | you should get a final speed of 63 .75 m/s | |
08:01 | . So this is the speed of the object opposition | |
08:04 | being . If there's no friction , now let's move | |
08:08 | on to part being what is the final speed of | |
08:11 | the block opposition B After traveling a total distance of | |
08:14 | 500 m , given a coefficient of kinetic friction Of | |
08:19 | .21 between the block and the surface . Now I | |
08:22 | do want to modify this . So let's say that | |
08:25 | the distance is only for the horizontal portion of the | |
08:30 | incline . So let's say that distance is 500 m | |
08:35 | , so not the total part . So let's say | |
08:38 | this portion , it's frictionless And the 500 m is | |
08:42 | only for the horizontal portion of the surface . Knowing | |
08:49 | that how can we calculate the final speed of the | |
08:51 | block ? A friction only acts on the bottom of | |
08:54 | the incline . So how can we modify this equation | |
09:02 | ? Opposition A . We're still going to have potential | |
09:05 | and kinetic energy . Now once you add friction to | |
09:09 | the mix the final speed will no longer be 63.75 | |
09:13 | , it's going to be less . So some of | |
09:17 | the energy from the left side is not all going | |
09:19 | to go into kinetic energy , some of it is | |
09:22 | going to go into the work done by friction . | |
09:25 | Now if you put the work done by friction on | |
09:27 | the left side it's going to be negative W because | |
09:29 | friction is going to decrease um the total energy of | |
09:33 | the object . And if it's negative W . On | |
09:36 | the left side then it's positive W . On the | |
09:38 | right side . So this represents the work done by | |
09:41 | friction frictions . Job is to take away the mechanical | |
09:46 | energy of the object and to convert it to thermal | |
09:49 | energy . So the energy loss from the object it's | |
09:54 | going to be W . And that amount of energy | |
09:56 | is going to be converted to heat energy . So | |
10:01 | let's go ahead and calculate w . 1st . So | |
10:14 | the work done by friction is equal to the kinetic | |
10:18 | friction of force . Times the distance that the force | |
10:21 | acts over distance and displacement are the same if the | |
10:26 | object doesn't change direction . So this work is force | |
10:30 | times displacement . Now the frictional force is equal to | |
10:36 | U . K . Times the normal force . So | |
10:40 | we have the coefficient of kinetic friction and the normal | |
10:44 | force on a horizontal surface is MG . Now if | |
10:49 | this part had friction that would complicate the problem because | |
10:52 | the normal force on let's say an incline is MG | |
10:57 | co signed data and this is not a straight incline | |
11:01 | so the angle changes . So that's just going to | |
11:03 | make it more complicated . So let's keep the problem | |
11:06 | simple . So now let's go ahead and calculate the | |
11:11 | work done by friction . So it's um UK . | |
11:13 | Which is 0.21 Multiplied by the mass of the object | |
11:17 | which is 10 times gene Times the distance that the | |
11:21 | object acts over which is 500 m . So let's | |
11:26 | multiply point to one by 10 By 9.8 and by | |
11:31 | 500 . So you should get 10,000 290 jewels . | |
11:41 | So that's the work done by friction . Now let's | |
11:47 | use that to calculate the final kinetic energy and also | |
11:51 | the final speed . So the potential energy is M | |
11:55 | . G . H . And the kinetic energy opposition | |
11:58 | A . Is one half and the initial square And | |
12:02 | the final Kinetic energy is 1/2 and the final square | |
12:06 | and then plus w . So let's plug in the | |
12:23 | values that we have . So the potential energy is | |
12:25 | gonna be 10 Time is 9.8 Times the height of | |
12:29 | 200 . And the initial kinetic energy is gonna be | |
12:33 | 1/2 times 10 times the initial speed which is 12 | |
12:40 | m/s . And then that's going to be the final | |
12:44 | kinetic energy . Plus the work done by friction which | |
12:50 | we can replace that with 10,290 jewels . So 10 | |
12:56 | times 9.8 times 200 That's 19,600 jewels . So there's | |
13:03 | enough potential energy to satisfy the work done by friction | |
13:07 | . Which tells us that The final speed is going | |
13:11 | to be greater than 12 . If this was less | |
13:15 | than friction , the final speed will be less than | |
13:16 | 12 . Now , let's multiply .5 x 10 by | |
13:21 | 12 square . So the kinetic energy of the object | |
13:24 | is very low . It's 720 . Make sure that's | |
13:29 | right . And yeah , that's it . So now | |
13:40 | let's add 19,600 plus 7:20 Unless subtract it by 10,290 | |
13:48 | . So the final kinetic energy is 10,030 jewels . | |
13:54 | So now let's set that equal to 1/2 MV final | |
13:58 | square . So we have one half times a massive | |
14:04 | 10 times the final square . So half of tennis | |
14:09 | , five and 10,030 divided by five is 2006 . | |
14:15 | So the square of the final speed is 2006 . | |
14:19 | Now let's take the square root of that number . | |
14:22 | So the final speed is going to be 44 0.8 | |
14:27 | meters per second , which was less than the final | |
14:31 | speed in part a a 12 kg block , moving | |
14:34 | at a speed of 15 m per second , crashes | |
14:38 | into a wall and comes to a complete stop . | |
14:41 | How much thermal energy was produced during the collision . | |
14:46 | So let's draw a picture . So , imagine you | |
14:48 | have a a block that sliding , It's moving at | |
14:52 | a speed of 15 m/s And it's a 12 kg | |
14:56 | mass , and then it collides with a wall . | |
15:02 | So once it hits the wall it comes to a | |
15:04 | stop . So it's no longer moving . Where did | |
15:07 | all of the kinetic energy go during collisions whenever you | |
15:12 | have an object in motion and then it's no longer | |
15:15 | in motion . You need to realize that the kinetic | |
15:18 | energy of that object was transformed into thermal energy , | |
15:22 | it's lost due to heat , and that heat just | |
15:25 | radiates outward into the surroundings . Think of let's say | |
15:31 | if you rub your hands quickly , you're going to | |
15:33 | feel that your hands start to get hot . So | |
15:36 | all of that kinetic energy that you are that your | |
15:39 | hands had as was moving back and forth . A | |
15:42 | lot of it was converted to thermal energy and so | |
15:44 | he was generated and that's what's going to happen here | |
15:48 | when that block collides with the wall and both objects | |
15:52 | where the wall is not moving , but the block | |
15:54 | comes to a stop . All of the kinetic energy | |
15:57 | that the bloc had was transferred to thermal energy . | |
16:03 | So let's calculate the initial kinetic energy of the block | |
16:06 | . So it's one half MV squared . So that's | |
16:10 | one half times a massive 12 kg Time to speed | |
16:16 | of 15 m/s . So half of 12 , 6 | |
16:20 | and 15 squared is to 25 Six times 2 25 | |
16:28 | is 1350 . So 13 15 jewels of kinetic energy | |
16:35 | was transformed into thermal energy . So that's the answer | |
16:40 | . No , let's move on to this problem . | |
16:43 | A 1500 kg car Moving east at 35 m/s , | |
16:49 | Crashes head on into another 1800 kg car . Moving | |
16:53 | west at 30 m/s , causing both cars to come | |
16:57 | to a complete stop . So let's turn this into | |
17:00 | a picture . So this is the 1500 kg object | |
17:07 | . It's a car , but I'm just going to | |
17:08 | draw a box and it's moving east At 35 m/s | |
17:14 | . And then we have another Object which is 1800 | |
17:18 | kg and this vehicle is moving west At 30 m/s | |
17:30 | . So they collide and they come to a complete | |
17:32 | stop . So all of the kinetic energies of these | |
17:36 | two objects that they once had , all of that | |
17:39 | was converted to thermal energy . So to calculate the | |
17:42 | total thermal energy produced , we need to calculate the | |
17:46 | total kinetic energy which is the kinetic energy of the | |
17:51 | first object . I'm going to call the object A | |
17:53 | . Plus the kinetic energy of the . Excuse me | |
17:57 | , The second object object B . So let's call | |
17:59 | this A . And B . So this is going | |
18:03 | to be 1/2 M . V . Squared plus one | |
18:07 | half M . V . Squared . So the mass | |
18:12 | of the first object is 1500 And it has a | |
18:14 | speed of 35 m/s . The mass of the second | |
18:18 | object is 1800 And it has a speed of 30 | |
18:23 | m/s . So .5 times 1500 times 35 squared . | |
18:31 | That's 918,000 750 jewels . And then .5 times 1800 | |
18:40 | times 30 . Swearing Is 810,000 jewels . So if | |
18:46 | we add these two numbers , This will give us | |
18:51 | one million 728,000 750 jewels . So that's how much | |
18:59 | thermal energy was produced during this collision . Consider this | |
19:07 | problem . So we have a roller coaster that's released | |
19:10 | from rest at .8 . How fast is it moving | |
19:15 | at point B . So how can we find the | |
19:19 | speed at point B . We need to use conservation | |
19:23 | of energy at 0.8 . The roller coaster has potential | |
19:27 | energy at point B . All of that potential energy | |
19:31 | is converted to kinetic . So let's set the potential | |
19:35 | energy , appoint a equal to the kinetic energy of | |
19:38 | the roller coaster at point B . So we have | |
19:41 | M . G . H . Will equal 1/2 Mv | |
19:45 | swear . So we could divide both sides by em | |
19:50 | . And then if we multiply both sides by tune | |
19:53 | , we're gonna have to G . H . Is | |
19:55 | equal to One half times two is once . So | |
19:58 | it's just going to be v . Squared . So | |
20:02 | the velocity , it's going to be the square root | |
20:05 | Of two G . H . So it's going to | |
20:09 | be the square root of two Times 9.8 . Multiplied | |
20:14 | by the height which is 50 . So let's go | |
20:19 | ahead and plug this in . So you should get | |
20:27 | 31.3 meters per second at point B . So that's | |
20:33 | how fast the roller coaster is moving at point B | |
20:37 | . If there's no friction in this problem now no | |
20:39 | friction was mentioned . So we're assuming there's no friction | |
20:55 | . Now it looks like I forgot to write part | |
20:57 | B . So we're going to move on to part | |
21:00 | Scene . How high is point C . Relative to | |
21:03 | point B . And I forgot to give you the | |
21:05 | speed at point C . To point seen . The | |
21:10 | speed Is 20 m/s . So with that information calculate | |
21:18 | the height of the roller coaster appoint scene , Point | |
21:25 | B . Is ground level . So how high is | |
21:27 | the point C . Feel free to pause the video | |
21:30 | . So I'm going to focus on point A . | |
21:33 | As my initial point . So the .8 all we | |
21:37 | had to begin with for its potential energy appoint scene | |
21:41 | . The object is above ground level . So it | |
21:44 | has potential energy now it's still moving at point C | |
21:49 | . So it also has kinetic energy . So we | |
21:53 | need to start with this expression . So we have | |
21:55 | M . G . H . This is gonna be | |
21:57 | a church initial is equal to MGH final plus one | |
22:03 | half M . V . Final square . Now we | |
22:08 | can divide every turn by em . And so we | |
22:11 | have this expression G . H . It's equal to | |
22:15 | G . H . Final plus one half the final | |
22:20 | square . So now let's plug in the numbers . | |
22:24 | It's going to be 9.8 Times the initial height which | |
22:28 | is 50 . And that's equal to 9.8 times the | |
22:32 | final height which is what we're looking for . And | |
22:37 | then plus 1/2 the final square the final at Point | |
22:43 | c . s . 20 . So 9.8 times 50 | |
22:48 | . That's 490 . And so that's equal to 9.8 | |
22:52 | times h . And 20 squared is 400 . Half | |
22:57 | of that is 200 Now 4 90 -200 is 2 | |
23:01 | 90 . So let's take 2 90 . Unless divided | |
23:06 | by 9.8 . Still 29 0.59 is equal to age | |
23:14 | . So that's how high it is at point C | |
23:21 | . Now let's move on to part D . How | |
23:24 | fast is the roller coaster moving ? Uh pointy . | |
23:28 | Mhm . So we're still gonna use part I mean | |
23:33 | .8 as our initial point . So at point A | |
23:38 | we still have initial potential energy at Point Dean . | |
23:43 | We still have potential energy because it's above ground level | |
23:46 | has the ability to fall . And that point D | |
23:50 | . It's still moving so it has kinetic energy . | |
23:53 | So we're gonna have the same equation . M . | |
23:56 | G . H . Initial is equal to MGH final | |
24:02 | plus one half M . V . Final square . | |
24:07 | And just like before we could cancel them . So | |
24:11 | G . is 9.8 . H . initial is still | |
24:15 | 50 Now H Final is now 15 . So the | |
24:20 | difference between part D . And part C . Is | |
24:25 | that in part D . We're looking for the final | |
24:27 | speed now . So 9.8 times 15 . That's still | |
24:33 | 4 90 . And that's equal to 9.8 times 15 | |
24:39 | Which is 1 47 . Yeah . Now let's take | |
24:48 | 4 90 and subtracted by 147 . So that's going | |
24:54 | to be 343 Is equal to 1/2 the final square | |
24:59 | Now multiply both sides by two . So 3 43 | |
25:03 | times two is 686 , 1/2 times two is 1 | |
25:07 | . So this is equal to the square of the | |
25:10 | speed . And now let's take the square root of | |
25:14 | both sides . So the square root of 686 is | |
25:21 | 26.19 meters per second . So that's how fast the | |
25:27 | roller coaster is moving at pointing . At that point | |
25:33 | . It was moving at 20 and that point , | |
25:35 | but it was like 30 something . So that's how | |
25:40 | you could solve the roller coaster problem using conservation of | |
25:43 | energy . |
Summarizer
DESCRIPTION:
This physics video tutorial explains how to solve conservation of energy problems with friction, inclined planes and springs.
OVERVIEW:
Conservation of Energy Physics Problems is a free educational video by The Organic Chemistry Tutor.
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