SAT Math Part 17 - Solving Formulas For a Specified Variable - By The Organic Chemistry Tutor
Transcript
00:0-1 | right 58 . The gravitational potential energy of an object | |
00:05 | is directly proportional to the mass of an object , | |
00:09 | as well as the gravitational acceleration of the planet and | |
00:14 | the height of the object above the ground . The | |
00:17 | formula is shown below which of the following expressions correctly | |
00:22 | represents the height of the object above ground level . | |
00:28 | Now something that you need to be able to do | |
00:30 | is you need to know how to solve for a | |
00:33 | certain variable in an equation . So in this case | |
00:38 | we want to solve for the height H . How | |
00:42 | can we isolate age in this equation ? So what | |
00:46 | we need to do is we need to divide both | |
00:49 | sides by M . G . So that diesel cancer | |
00:54 | . So age is going to equal to what we | |
00:56 | see on the left . It's the gravitational potential energy | |
01:00 | you divided by the mass and divided by the gravitational | |
01:05 | acceleration of the planet . So this represents the height | |
01:09 | of the object , which means that answer choice A | |
01:12 | is the correct answer . 59 . The final velocity | |
01:18 | of a moving vehicle is equal to the sum of | |
01:22 | the initial velocity and the product of its acceleration and | |
01:26 | time , which is the following expressions represent the acceleration | |
01:32 | of the moving vehicle . So we need to isolate | |
01:37 | the variable a acceleration . How can we do some | |
01:42 | ? Yes . We need to get a by itself | |
01:45 | somehow . Now what we need to do in order | |
01:49 | to do this is subtract both sides by the initial | |
01:53 | , so we're going to have the final minus the | |
01:57 | initial Is equal to 18 . Now we need to | |
02:01 | separate A from T . Since they're multiplied to each | |
02:04 | other , we need to divide so let's divide both | |
02:08 | sides by T . So the acceleration is the final | |
02:13 | velocity minus the initial velocity , which is basically the | |
02:18 | change in velocity divided by the time . So this | |
02:22 | right here is our answer , which corresponds to answer | |
02:25 | choice B . Number 60 . The combined gas law | |
02:30 | equation shown below describes the relationship between the pressure volume | |
02:36 | and Calvin temperature of an ideal gas , Which of | |
02:40 | the following expressions can be used to calculate T . | |
02:43 | two . So here we have two fractions separated by | |
02:50 | an equal sign . Something that we can do is | |
02:53 | cross multiply . So this will give us P two | |
02:57 | V two times T one , And that's going to | |
03:00 | be equal to P one if he wanted T to | |
03:04 | . Now , in this form , it's going to | |
03:06 | be very easy to isolate teach you all we need | |
03:09 | to do is divide both sides By P one . | |
03:12 | V . 1 . Yeah . And so T two | |
03:16 | is equal to what we see on the left side | |
03:19 | . It's P two V 2 , T one Over | |
03:22 | P one V 1 , which means answer choice D | |
03:25 | . Is the answer 61 . The electric force between | |
03:31 | two charged particles is proportional to the magnitude of each | |
03:36 | electric charge and inversely proportional to the square of the | |
03:42 | distance between the center of the charges . Which equation | |
03:48 | can be used To calculate the magnitude of the first | |
03:51 | charge Q one . So how can we isolate Q | |
03:57 | one in this problem ? What's the first thing that | |
04:02 | we need to do ? What I would recommend is | |
04:06 | multiplying both sides by R squared . So on the | |
04:10 | right side these will cancel . Next we can divide | |
04:16 | both sides by K and Q tune . Yeah . | |
04:23 | Yeah . So cable cancel and Q two will cancel | |
04:28 | . So all we have left over on the right | |
04:30 | side is Cuban . So Q one is equal to | |
04:33 | F . Times are squared divided by K and divided | |
04:38 | by Q two , which means A . Is the | |
04:41 | right answer . Choice 62 . The gravitational force between | |
04:47 | two planets is directly proportional to the mass of the | |
04:51 | planet and inversely related to the square of the distance | |
04:56 | between their centers . Which equation can be used to | |
05:01 | calculate art . So how can we isolate are in | |
05:08 | this equation ? Well , first we don't want it | |
05:14 | to be on the bottom of a fraction . So | |
05:16 | let's multiply both sides by our square . Yeah . | |
05:22 | Now the next thing we want to do is divide | |
05:24 | both sides by F . So right now we have | |
05:29 | R squared is equal to G . M one M | |
05:33 | 2 Over F . Now to get rid of the | |
05:36 | square , we need to take the square root of | |
05:39 | both sides , so the square root of R squared | |
05:43 | is simply are so R is equal to what we | |
05:48 | see here , which means that De is the right | |
05:51 | answer . 63 . The difference in pressure between two | |
05:58 | points and a moving fluid depends on the density of | |
06:02 | the fluid . The height difference between the two points | |
06:06 | and The fluid velocities V two and V one of | |
06:10 | those two points , according to Bernoulli's equation , which | |
06:15 | of the following expressions can be used to calculate the | |
06:18 | density of the fluid . So the density of the | |
06:22 | fluid is represented by the greek symbol role , which | |
06:26 | looks like a lower case P . Now we need | |
06:29 | to isolate the role , but there's two of them | |
06:32 | . So what should we do whenever you want to | |
06:36 | isolate a variable ? And if you have more than | |
06:39 | one of that variable , what you need to do | |
06:41 | is factor . So we're going to factor out the | |
06:45 | density . So if we take out roll from rogue | |
06:49 | , ehh it's gonna be just negative G . H | |
06:53 | . And if we take out road from this expression | |
06:55 | , it's gonna be everything acceptable . So this is | |
07:03 | what we now have . The last thing that we | |
07:06 | need to do is divide both sides by what we | |
07:10 | see here . That is by negative G . H | |
07:15 | minus one half V . Two minus V . One | |
07:17 | squared . And let's do the same on the left | |
07:22 | side . So on the right side all of this | |
07:31 | will disappear . So all we have left over on | |
07:34 | the right side is the density rho on the left | |
07:38 | is the answer . So this corresponds to answer choice | |
07:43 | A . 64 . So here we have the simplified | |
07:48 | version of the Doppler effect formula . And it describes | |
07:53 | the relationship between the frequency of sound measured by a | |
07:57 | stationary observer . That is fo emphases basically the source | |
08:03 | frequency , that's the object generating the source . I | |
08:08 | mean the object generating the sound and V . Represents | |
08:14 | the speed of sound in the air . V . | |
08:17 | S . Is the speed of the object generating the | |
08:21 | sound . So in this problem we want to determine | |
08:25 | the speed of sound and air . We need to | |
08:27 | isolate the variable V . So how can we do | |
08:31 | that ? Especially since we have two of them . | |
08:35 | So at some point we need to factor out V | |
08:38 | . But we can't do that in its current form | |
08:42 | . So we're going to have to rearrange the equation | |
08:46 | . So let's begin . The first thing we need | |
08:48 | to do is multiply both sides by v minus vitas | |
08:55 | . So on the right side , these will cancel | |
08:59 | . So right now , what we have left over | |
09:01 | is V minus V . S . Times fo and | |
09:06 | that's equal to the product of these two V times | |
09:09 | FFS mm . Our next step is to distribute fo | |
09:20 | so we have fo times V . And then fo | |
09:24 | times of the S . Yeah , now I'm going | |
09:33 | to take this term , move it to the other | |
09:35 | side . It's negative on the left side , but | |
09:38 | it's going to be positive on the right side . | |
09:41 | And this term I'm going to move it to the | |
09:43 | left side , it's positive on the right , but | |
09:45 | it will be negative on the left . So if | |
09:48 | you want to show your work , we're going to | |
09:51 | add V . S . F . O . To | |
09:55 | both sides , and at the same time we're going | |
09:57 | to subtract VF F s from both sides . Yeah | |
10:02 | . Mhm . So we're gonna have the F . | |
10:05 | O minus V . F . S . And that's | |
10:09 | equal to V . S . F . O . | |
10:12 | Our next step is to factor out with the , | |
10:18 | so if we take out V we're going to have | |
10:21 | F . O minus F . S and then that's | |
10:23 | equal to V . S . Fo Yeah , so | |
10:28 | that's how we can take out or convert to v | |
10:31 | variables into one . It's by factor in that . | |
10:34 | Our next step is to the viable size by f | |
10:36 | o , f s or fo minus f s . | |
10:41 | Yeah , so now we have our final answer . | |
10:44 | V is equal to what we see on the right | |
10:46 | side , which means as a choice , C is | |
10:49 | the right answer . |
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