How many times have you seen a cat walk in the path of x²? Almost never. Cats (like Salem) pounce, jump, and walk in circles. However, there are no functions to describe Salem’s movement. By incorporating time into a function, parametric equations allow us to describe these paths of movements that we could not describe before. One function relies on time, t, to describe the movement with respect to x, and the other function relies on time, as well, to describe the movement with respect to y. Together, they give you graphs that can describe movement we could not describe before like the movement of the eight ball as Cory and Shawn play pool or the path of Forman’s smoke.
Mustapha Amrani is a professor at the University of Cambridge and is affiliated with the Isaac Newton Institute. He studies parametric equations in detail so as to find real-world applications for the concept and he gives talks on his findings. Amrani has discovered a use of parametric equations that was previously unknown-- he has begun to incorporate parametric equations and semi-parametric equations into electricity consumption forecasting. For utilities it is necessary to have a good idea of the future's electricity consumption and Armani has found that through the use of parametric equations in his work he is able to better predict the consumption trends that will occur thereby aiding the utilities. Since Armani uses primarily semi-parametric structures he is able to create an even more accurate prediction as his models create a complex but interesting trade-off between previous accurate forecasts and new adaptations to different data sets. Although these contributions are still gaining credibility and usage in the real-world, Armani has proven how parametric equations can be utilized with a multitude of different geographical climates and horizons in order to try to accurately predict the electricity consumption of the future.
First, let’s learn how to eliminate the parameter. Eliminating the parameter allows for you to go from parametric equations to polynomial equations. Ultimately we are eliminating time, t, from the equation. So, when told to eliminate the parameter, look at the x - and-y functions and decide in which equation would it be easier to solve for time, t. Although both of the equations above are quite messy, the y-equation seems to be easier to solve for time, t. The last step is to solve for time, t, in the y-equation and plug it in for time, t, in the x-equation. You just eliminated the parameter! Wasn’t that easy?
Graph and find the equation of the tangent line to the graph at t=1 if x(t)=2t²-4 and y(t)=t²-3t+1 First, let’s graph the parametric equation! tx(t)y(t) Graphing parametric equations are quite different from regular equations. Because the equations are given with respect to time, we are actually calculating positions at certain times. So, you would want to create a table of values like the one to the bottom-left and graph the points by plugging time into the x- and y-functions. For example, at t=0, the x-value is -4 and the y-value is 1. So, the first point will be (- 4,1). Continue this with the rest of the points. Also, one thing greatly different from regular graphs is direction. So add an arrow to specify what direction you are going.
Now, it’s time to find the tangent line! When finding tangent lines, it’s not too different from regular equations. First, find the derivatives of both x- and y- functions. Next, it’s time to find the slope of the tangent line. But, how do we do this when we have two functions!?!? You simply divide the derivative of the y-function by the derivative of the x-function. Now that we have the slope of the tangent line, it’s time to find the x- and y-coordinates. This step is a bit more straight forward. Just plug in t=1 into the functions!
Finally, it’s time to put it all together and graph the tangent line! Now you know how to graph parametric equations and find their tangent lines!
To find a vertical tangent line, we must solve for when the derivative of the x-function is equal to zero. This will give us the time at which there is no movement in the x-direction and thus a vertical tangent line! a. 0 c. 2
We now have the two times at which there is no movement in the x-direction. So we’re done now right!? Well not quite. We have to test these times in the derivative of the y-function and make sure it does not equal zero. Why may you ask? Well, what’s happening to the graph when both the derivative of x and y are zero? That’s right, nothing. There’s no movement, and therefore, there wouldn’t be a vertical tangent line at that moment.
Once you hear the word concavity, immediately think the second derivative! Wait, but how do we take the second derivative of a parametric function? First we find the first derivative which we already learned how to do. Differentiate the x- and y-functions then set dy over dx. This is the first derivative. Now differentiate the first derivative to get the second derivative, but wait a second! The second derivative is in terms of dt! It should be in terms of dx ² ! To solve this problem just divide the second derivative we just found by dx. Then evaluate at t=-3! Because the second derivative evaluated at t=-3 is greater than zero than the graph is concave up!
To find the distance the eight ball traveled, we will want to use the arc length equation. So first, we need to find the derivatives of the x- and y-functions. Now just plug in the derivatives into the arc length equation and solve it by using your graphing calculator!
The eight ball that Eric hit traveled a total distance of inches!
Eliminate the parameter: 2) Graph the following parametric equations: 4) 5) 6) 7)8)
Find the tangent line: 9) At t=2:10) At t=1: 11) At t=3: (A) (B) (C) (D) (E)
pg_gen/derivatives/landscape_635/article-boymeetsworld-1127.jpg jpg mage/image.jpg_gen/derivatives/gallery_635/70-show.jpg sabrina-the-teenage-witch _1920_1536.jpg 03boy-meets-world1_300x206.jpg https://i.chzbgr.com/maxW500/ /hF1B775DE/ Multiple-Choice & Free-Response Questions in Preparation for the AP Calculus (BC) Examination by David Lederman