Kinematics In One Dimension - Physics - By The Organic Chemistry Tutor
Transcript
00:01 | in this video , we're going to talk about schematics | |
00:04 | , which basically describes how objects move without any references | |
00:09 | to force . Now we're going to focus on schematics | |
00:13 | in one dimension , mostly along the X axis , | |
00:18 | but we can also work on some problems along the | |
00:20 | Y axis . When you get into two dimensional mathematics | |
00:24 | , it covers project emotion , which is a topic | |
00:28 | for another day . Now the first thing we need | |
00:31 | to talk about is the difference between a scale of | |
00:35 | quantity and a vector quantity . A scale of quantity | |
00:42 | is something that has magnitude only , whereas a vector | |
00:46 | quantity has both magnitude and direction . So for instance | |
00:53 | , mass is a scalar quantity . You could say | |
01:00 | that a book has two kg of mass And the | |
01:04 | two kg Would be the magnitude of the mass of | |
01:08 | the book . But you wouldn't say the book has | |
01:11 | two kg of mass . East direction wouldn't apply for | |
01:16 | mass . So mass cannot be a vector quantity . | |
01:23 | Distance is a scale of quantity and displacement is a | |
01:31 | vector quantity , displacement . You can think of it | |
01:36 | as distance with direction . So let's say if a | |
01:41 | person traveled 15 m , you're basically describing a person's | |
01:46 | distance because you didn't mention direction . But let's say | |
01:50 | if someone traveled 15 m east now you're describing displacement | |
01:55 | . You describe in not only how far he traveled | |
01:59 | , but also where he traveled . So think of | |
02:01 | displacement as distance with direction . Now technically displacement is | |
02:07 | really the change in the position of an object . | |
02:12 | So along the X axis you could describe displacement as | |
02:15 | the final position , modest the initial position , speed | |
02:23 | is a scale of quantity . Speed describes how fast | |
02:27 | an object is moving . Velocity is a vector quantity | |
02:33 | , velocity is speed with direction . So if you | |
02:37 | were to say , a person is traveling at uh | |
02:41 | 20 m/s , you're describing the speed of the person | |
02:44 | , this is the magnitude . But let's say if | |
02:47 | a person is moving at 30 m/s north , you're | |
02:52 | describing velocity because you've mentioned his speed along with the | |
02:58 | direction . So you have both magnitude and direction , | |
03:01 | which makes it a vector quantity . Now , what | |
03:05 | about temperature ? Would you say that temperature is a | |
03:10 | scale of quantity ? Or would you describe it as | |
03:12 | a vector quantity ? So , think of units of | |
03:18 | temperature . Let's say it's a 80°F outside Or 25°C. | |
03:27 | . You wouldn't say it's 80°F direction doesn't apply for | |
03:32 | temperature . So because you can't describe the direction of | |
03:36 | temperature , it's not relevant . Temperature is a scale | |
03:40 | equality . You can only mention its magnitude , such | |
03:46 | as how hot it is , 80°F. . But you | |
03:50 | can't attach direction to temperature , which makes it scaler | |
03:54 | now acceleration and that is a vector quantity , acceleration | |
04:04 | tells you how fast the velocity changes . And you | |
04:08 | could say a car is accelerating at two m per | |
04:12 | second squared east , you can put direction to it | |
04:16 | . So acceleration is effective quantity . Now let's talk | |
04:21 | more about the difference between distance and displacement . So | |
04:29 | let's say a person walk , Let's say a person | |
04:34 | traveled 13 m east and then he turns around And | |
04:41 | travels four m west . We're going to add a | |
04:46 | negative science this because he's going towards the left and | |
04:51 | just to review direction north and south is along the | |
04:54 | Y axis , east and west there along the X | |
05:00 | axis . So peace is along the positive X axis | |
05:05 | . West is along the negative X axis . So | |
05:10 | given a situation , calculate the distance and the displacement | |
05:15 | of this individual that traveled here . Let's put a | |
05:20 | person . So the total distance that this person traveled | |
05:32 | is 17 m . Mhm . It's basically the some | |
05:38 | of these two numbers he traveled 13 m east and | |
05:41 | then four m west . So a total distance of | |
05:44 | 17 m distance being scalar , it's always positive . | |
05:52 | Now there is an exception to this , specifically temperature | |
05:56 | depending on the units you're dealing with . Even though | |
06:00 | temperatures , the scale of quantity , you could have | |
06:01 | negative values , especially for units such as Fahrenheit and | |
06:06 | Celsius . So some places can be negative 20°F in | |
06:12 | temperature , Others negative 10°C. . But on the kelvin | |
06:17 | scale there's no negative values . So there are some | |
06:21 | scalar quantities that do have negative values like temperature . | |
06:24 | So just be aware of that . Now , going | |
06:28 | back to this problem , now that we know the | |
06:30 | total distance traveled , what is the displacement of this | |
06:35 | particular individual ? Now , displacement can be positive or | |
06:41 | negative dependent on the direction . If you were to | |
06:46 | combine these two , including the negative four value , | |
06:49 | It would be 13 -4 , So the displacement is | |
06:53 | positive . nine , displacement is the final position minus | |
06:59 | the initial position . So displacement is the change in | |
07:03 | position . What this tells us is that This person | |
07:08 | ended up nine m east from where he started . | |
07:12 | And so let's illustrate this with a number line . | |
07:16 | So let's say that He started at the origin position | |
07:20 | zero . He traveled 13 m east . So because | |
07:26 | he's moving along the positive X axis , we assign | |
07:29 | a positive value here . And then during the second | |
07:33 | part of his trip He traveled four m west . | |
07:38 | So 13 -4 . He ends up at position nine | |
07:44 | . So the net result is that he traveled nine | |
07:48 | m east and so that's his displacement . That's how | |
07:52 | far he traveled relative to his in his initial position | |
07:58 | . So hopefully this example gave you a good understanding | |
08:01 | between the difference of distance and displacement . So remember | |
08:05 | , distance is a scale of quantity . It's always | |
08:08 | positive and displacement is a vector . It has both | |
08:13 | magnitude and direction . Now let's talk about the difference | |
08:17 | between speed and velocity . Remember speed is a scale | |
08:23 | of quantity but velocity is a vector quantity , speed | |
08:29 | has magnitude only , but velocity has both magnitude and | |
08:32 | direction . Let's use s to describe speed as would | |
08:39 | represent the instantaneous speed . That is how fast an | |
08:42 | object is moving at an instant of time . But | |
08:45 | S . Bar represents the average speed . Average speed | |
08:50 | is equal to the distance traveled divided by the time | |
08:57 | that was elapsed , average velocity is equal to displacement | |
09:06 | over time . So therefore speed is always positive . | |
09:16 | Velocity can be positive or negative depending on the direction | |
09:23 | . So average velocity is basically the velocity calculated over | |
09:27 | a time interval . Now let's use an example to | |
09:31 | calculate speed . I mean average speed and average velocity | |
09:34 | . So let's say we have a particle and this | |
09:37 | particle Travels 100 m east And then it turns around | |
09:46 | and travels 150 m west and it does all of | |
09:53 | this in five seconds , calculate the average speed and | |
10:00 | the average velocity of this particle Over this 5 2nd | |
10:05 | time interval . So to calculate the average speed first | |
10:11 | , we need to calculate the total distance traveled . | |
10:15 | This particle traveled a total distance of 250 m . | |
10:20 | It traveled 100 m east and then 100 and 50 | |
10:23 | m west . So if you add those two numbers | |
10:26 | , you get a total distance of 250 m . | |
10:30 | Now it did this in five seconds to 50 , | |
10:33 | divided by five is 50 . So the average speed | |
10:38 | Of this particle is positive 50 m/s . Now the | |
10:46 | average velocity is different because the displacement is different . | |
10:52 | Now there's two ways in which we can calculate the | |
10:54 | displacement . We can add up the individual the displacements | |
11:00 | for the individual segments of the problem . The displacement | |
11:04 | for the first part is a 100 m And the | |
11:07 | displacement for the second part is -150 . If we | |
11:11 | add 100 plus negative 150 we get In that displacement | |
11:16 | of -50 . The other way in which you can | |
11:20 | calculate displacement is by taking the final position and subtracted | |
11:25 | by the initial position and it helps to draw a | |
11:28 | number line for this . So the particles started opposition | |
11:32 | zero . And during the first part of this traveled | |
11:38 | It was at position 100 And then it traveled 150 | |
11:42 | m west , so it ended at position -50 . | |
11:48 | So its final position was negative 50 Minour its initial | |
11:53 | position of zero , Which will still be negative 50 | |
11:58 | . I mean you could do it that way too | |
11:59 | , but I prefer to simply add the displacement of | |
12:04 | each individual part of the problem to get the final | |
12:07 | displacement . So the final displacement is negative 50 m | |
12:14 | Divided by a time of five seconds . So negative | |
12:17 | 50 divided by five . The average velocity Calculated is | |
12:23 | negative 10 m/s . So as you can see the | |
12:29 | average speed and the average velocity is not always the | |
12:34 | same , it's going to be the same if the | |
12:39 | person or the object travels in one direction , but | |
12:42 | if there's any change in direction , like when this | |
12:45 | particle you know decided to go west , that's when | |
12:50 | the average speed and the average velocity will be different | |
12:55 | . So keep in mind the average speed doesn't have | |
12:58 | to equal the average velocity . Sometimes they are equal | |
13:02 | to each other , but it's not always the case | |
13:07 | now for instantaneous speed that is the absolute value of | |
13:11 | instantaneous velocity . The instantaneous velocity tells you the velocity | |
13:16 | at an instant of time where is the average velocity | |
13:21 | basically tells you the average over an interval . So | |
13:25 | remember average velocity is the displacement over time and displacement | |
13:30 | is the final position minus the initial position divided by | |
13:34 | t now instantaneous velocity in order to calculate it . | |
13:41 | You need to use limits . So it's to limit | |
13:44 | as the change in time goes to zero . And | |
13:48 | it's basically the displacement over time or the change of | |
13:53 | position over the change in time . So that's how | |
13:57 | you would calculate instantaneous velocity . Which we really won't | |
14:05 | go over that in this video . But for those | |
14:07 | of you who want the formula , that's what it | |
14:09 | is . And whenever you see delta this triangle , | |
14:15 | it represents the change of something in this case the | |
14:19 | change in position . So delta X . Is the | |
14:22 | final position minus the initial position . So basically it's | |
14:26 | the displacement along the X axis . But you can | |
14:31 | also have displacement along the y axis . In this | |
14:34 | case it will be the final position along the y | |
14:36 | axis , modest initial position . So whenever you see | |
14:41 | the symbol D , you could describe it using distance | |
14:46 | or displacement . Now let's talk about some formulas that | |
14:52 | you need to be familiar with when an object is | |
14:59 | moving with constant speed . Typically this is the formula | |
15:05 | that you need to work with . D . Is | |
15:08 | equal to VT . So in this equation D could | |
15:14 | represent distance or displacement depend on how you use the | |
15:18 | problem V . You could use speed or velocity . | |
15:25 | It's going to work if you're dealing with constant speed | |
15:29 | . But understand this story . If you're using V | |
15:32 | . S speed then D is going to be the | |
15:33 | distance . If you're using V with reference to velocity | |
15:38 | D . Is going to represent the displacement . Now | |
15:42 | for objects moving at constant speed , you need to | |
15:45 | know that the instantaneous velocity is the same as the | |
15:51 | average velocity because the velocity is not changing . So | |
15:55 | whether you use V or V bar it will have | |
15:58 | the same effect . Now let's talk about when objects | |
16:05 | are moving with constant acceleration . And by the way | |
16:15 | , remember if you're using displacement , displacement is the | |
16:22 | final position minus the initial position . But if you're | |
16:25 | dealing with distance , you don't have to worry about | |
16:26 | that . So just keep in mind if you're using | |
16:29 | Diaz displacement or distance now for constant acceleration , we | |
16:38 | have some formulas that we need to take into account | |
16:45 | for cause acceleration , D . Is equal to V | |
16:48 | bar times T . And the reason for that is | |
16:52 | that V doesn't equal V bar when this acceleration anytime | |
17:01 | this acceleration , that means the velocity is changing , | |
17:05 | acceleration tells you how fast the velocity is changing . | |
17:09 | And if the velocity is changing then the instantaneous velocity | |
17:13 | and the average velocity for most of the time won't | |
17:17 | be the same . So that's why we need to | |
17:26 | use V bar . Now the average velocity is the | |
17:32 | average of the initial velocity And the final velocity . | |
17:37 | So it's basically the some of the initial of the | |
17:39 | final velocity divided by two . Or you can fight | |
17:43 | it this way , 1/2 the initial plus of the | |
17:46 | final . So if we were to replace V Bar | |
17:52 | with this expression we would get The displacement is equal | |
17:56 | to 1/2 the initial plus of the final times . | |
18:02 | T . So remember if you're using Diaz distance , | |
18:09 | then the initial is the initial speed . The final | |
18:12 | is the final speed . But if you're using ds | |
18:15 | displacement , v . Initio is your initial velocity the | |
18:18 | final is your final velocity . So let's rewrite that | |
18:25 | equation here . This is one of those equations that | |
18:29 | you want to write in your list of equations . | |
18:33 | If you have a test coming up now there's some | |
18:36 | other equations that we're going to add to this list | |
18:40 | . So we said that average velocity is the displacement | |
18:45 | , which is final position minus initial position divided by | |
18:48 | T . Well , if you would have rearranged that | |
18:52 | equation , You'll get this one final position is equal | |
18:58 | to initial position plus the average velocity times T . | |
19:07 | You can also get it from this equation . D | |
19:10 | is equal to V . Bar times T . And | |
19:17 | D being the displacement is x final minus x . | |
19:20 | Initial . And so if you were to move this | |
19:24 | to that side , you would end up with the | |
19:29 | same equation . So there's many ways in which you | |
19:31 | can derive that equation . So that's the next one | |
19:34 | that you want to have in your list . Now | |
19:40 | we said that average velocity is the displacement or the | |
19:45 | change of position divided by the time , average acceleration | |
19:49 | is the change in velocity divided by time . It's | |
19:54 | the final velocity minus the initial velocity divided by T | |
19:59 | . So if you re arrange that equation , you | |
20:01 | get something similar to the one that we have above | |
20:04 | V . final is equal to the initial plus 80 | |
20:11 | . Now there are some other equations that we can | |
20:13 | add to the list . Another one is the final | |
20:17 | squared is equal to the initial squared Plus two times | |
20:21 | a . D . And then there's this one , | |
20:27 | displacement is equal to the initial T . Plus one | |
20:31 | half at squared . And any time you see the | |
20:35 | letter D . You can replace that with X . | |
20:37 | Final minus x . Initial . So if we were | |
20:41 | to substitute X final minus X . Initial for D | |
20:46 | . And then move X initial to the right side | |
20:48 | of the equation . We'll get this equation . Final | |
20:52 | position is equal to initial position plus the initial T | |
21:00 | . Plus one half a . T squared now because | |
21:05 | this is X . Where dealing with motion along the | |
21:08 | X axis . But when you go into project that | |
21:12 | motion you can apply motion along the Y axis as | |
21:17 | well . So you might see this variation of this | |
21:20 | formula Y final equals Y initial plus V . Y | |
21:25 | . Initial T . So that's initial velocity but in | |
21:28 | the Y direction plus one half A . T squared | |
21:32 | . Where A . Is like the gravitational acceleration in | |
21:36 | the right direction . So just understand that you can | |
21:43 | apply these formulas in the X . Direction or in | |
21:46 | the Y . Direction . So it might be a | |
21:49 | lot to keep track of . But as you begin | |
21:51 | to work problems , uh the use of these formulas | |
21:54 | will begin to make more sense . But you may | |
21:57 | want to write these down for your reference now , | |
22:00 | before we work on a few example problems , there's | |
22:03 | something I do want to mention when dealing with constant | |
22:05 | speed , you could use this formula X final is | |
22:09 | equal to X initial plus VT . So you don't | |
22:13 | need to survive V Bar because V and V bar | |
22:16 | are the same when dealing with constant speed . But | |
22:21 | for constant acceleration , it's good to keep in mind | |
22:26 | that this represents average velocity . So it's better to | |
22:33 | write V Bar instead of the so there's no confusion | |
22:35 | because these two , they're not necessarily the same when | |
22:39 | dealing with constant acceleration . So just be aware of | |
22:43 | that little detail , Let's start with this one . | |
22:47 | A bus is traveling at a constant speed of 40 | |
22:50 | m/s . How many hours will it take to travel | |
22:55 | ? A distance of 200 miles ? So what formula | |
23:00 | do we need to use ? So we're given the | |
23:04 | speed which we can use as a symbol , V | |
23:08 | or S . And we know the distance which is | |
23:15 | 200 miles . The only form of that we could | |
23:21 | use since the bus is moving at constant speed is | |
23:26 | this one . D . Is equal to VT . | |
23:30 | Now , before we use that formula , we need | |
23:33 | to take a look at the units . Here we | |
23:35 | have meters per second and here we have mouse and | |
23:40 | we want to find a time in hours . So | |
23:43 | we're looking for tea , the units they don't match | |
23:48 | . So before we could use the formula , we | |
23:50 | need to convert the units into an appropriate form . | |
23:54 | So what do you recommend that we need to do | |
23:58 | ? We have the distance in mouse and we want | |
24:01 | to find a time in hours . The best thing | |
24:04 | we can do is convert the speed from meters per | |
24:07 | second , two mph . Once we do that , | |
24:13 | then it will match with the unit hours and the | |
24:18 | unit mouse . So we can now use that formula | |
24:21 | . So let's go ahead and convert 40 m/s , | |
24:25 | two mph . So let's get an overview of how | |
24:31 | we're gonna do this . Let's convert meters , two | |
24:35 | km and then kilometers to mouse And then we're gonna | |
24:39 | convert seconds , two minutes and then minutes to hours | |
24:47 | . So in order to convert miles to kilometers , | |
24:49 | you need to know the relationship between the two . | |
24:52 | One kilometer is equivalent to 1000 m . I meant | |
24:58 | to say m instead of mouse , but that's how | |
25:00 | you can go from m two km . Now , | |
25:04 | these units cancel . Now let's convert from kilometers to | |
25:08 | mouse . So we need to put the unit kilometers | |
25:13 | on the bottom miles on top so that these units | |
25:17 | will cancel . You need to know that One mile | |
25:22 | is equal to 1.609 km . So now we have | |
25:27 | the unit Mouse , let's convert seconds , two minutes | |
25:31 | since we have seconds on the bottom , we want | |
25:33 | to put seconds on top and then minutes on the | |
25:36 | bottom , one minute is equal to 60 seconds . | |
25:41 | So now we can cross out this unit and now | |
25:47 | let's convert minutes to hours . one hour is equivalent | |
25:51 | to 60 minutes . And so we could cancel the | |
25:55 | unit minutes . So now let's do the math . | |
26:03 | We're going to multiply by all the numbers that are | |
26:06 | on the top . But we're gonna divide by the | |
26:08 | numbers on the bottom , So it's gonna be 40 | |
26:11 | , divided by 1000 . Take that result divided by | |
26:14 | 1.60.9 And then multiply that by 60 and then buy | |
26:19 | another 60 . So for the velocity or rather than | |
26:26 | speed You should get 89 .5 If you run it | |
26:34 | MPH which we can write mph . So that's how | |
26:40 | we can convert meters per 2nd 2 mph . Now | |
26:46 | let's go ahead and finish this problem . So let's | |
26:49 | use the formula D . Is equal to V . | |
26:51 | T . In this case D . is going to | |
26:55 | represent the distance which is 200 miles . V . | |
27:00 | is going to be the speed which is 89 0.5 | |
27:06 | MPH . And then now we can calculate team so | |
27:12 | he gets here by itself . We need to divide | |
27:14 | both sides By 89.5 MPH . 200 divided by 89.5 | |
27:36 | gives us this answer to point 23 hours . Now | |
27:44 | . Looking at the units , we can see that | |
27:46 | the unit miles cancel leaving behind the unit hours , | |
27:50 | which is , well , we want the final answer | |
27:53 | to be in . So when dealing with these problems | |
27:57 | , always check to make sure that the units match | |
28:01 | . If they don't match , you need to convert | |
28:03 | one unit into another . So just keep that in | |
28:06 | mind . Now let's move on the part B of | |
28:14 | this problem . If the bus moved from a position | |
28:17 | that is 50 miles east of city XY . Z | |
28:22 | . to a position that is 90 miles west of | |
28:25 | city X Y . Z . In five hours , | |
28:26 | what is the average velocity of the bus during that | |
28:29 | time in the vote ? So let's say this is | |
28:36 | City X , Y Z . So the bus was | |
28:43 | initially , let's say opposition , eh , which is | |
28:48 | 50 miles east of city . Ex wise , actually | |
28:54 | , that's wes , I take that back , Let's | |
29:03 | say city X , YZ is at the origin position | |
29:06 | zero . So the bus was 50 miles east of | |
29:10 | the city . So it was initially here . So | |
29:15 | this is going to be X initial , that's the | |
29:17 | initial position of the bus and then it moved To | |
29:23 | a position that is 90 miles west of that city | |
29:28 | . So this is gonna be -90 . That's the | |
29:31 | final position of the bus . So the buses traveling | |
29:38 | west , which means that the average velocity should be | |
29:42 | a negative value . Now , how can we calculate | |
29:48 | the average velocity ? What formula do we need to | |
29:51 | use ? It really helps to write down everything . | |
29:54 | We know that X initial is 50 X . Final | |
29:59 | is negative 90 and the units are in mouse and | |
30:08 | then we have the time , which is five hours | |
30:12 | . We want to calculate the average velocity . Well | |
30:16 | we know that average velocity is displacement over time and | |
30:20 | displacement is the change in position . X final minus | |
30:24 | X . Initial whenever you're dealing with motion along the | |
30:29 | X axis and then divided by the time . So | |
30:33 | the final position is -90 . The initial position is | |
30:37 | positive 50 . The time is five hours So -90 | |
30:45 | - positive 50 . That is -140 . So the | |
30:52 | change in position or a displacement that is negative 140 | |
30:58 | miles . And we're going to divide that by five | |
31:00 | hours . So 1 40 divided by five is 28 | |
31:05 | . Thus the average velocity , it's going to be | |
31:09 | negative 28 MPH which we can right as mph . | |
31:18 | So that's how we can calculate the average velocity for | |
31:21 | this particular problem . |
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