x and y coordinates at t=0 of the object
{"title":"x and y coordinates at time t of an object in projectile motion","description":"Wrong","type":"incorrect","color":"#99CCFF","code":"[{\"shape\":\"rect\",\"coords\":\"34,9,61,34\"},{\"shape\":\"poly\",\"coords\":\"82,133\"},{\"shape\":\"rect\",\"coords\":\"41,57,60,84\"}]"} {"title":"x and y component at t=0 of the object's velocity vector","description":"Incorrect","type":"incorrect","color":"#ffcc00","code":"[{\"shape\":\"rect\",\"coords\":\"118,11,119,13\"},{\"shape\":\"rect\",\"coords\":\"150,11,168,29\"},{\"shape\":\"rect\",\"coords\":\"143,55,162,79\"}]"} {"title":"Time at which the object has coordinates x and y","description":"Wrong","type":"incorrect","color":"#333300","code":"[{\"shape\":\"poly\",\"coords\":\"113,132\"},{\"shape\":\"rect\",\"coords\":\"183,7,203,32\"},{\"shape\":\"rect\",\"coords\":\"180,53,196,80\"},{\"shape\":\"rect\",\"coords\":\"278,48,293,78\"}]"} {"title":"Acceleration due to gravity (g is positive)","description":"Incorrect","type":"incorrect","color":"#000080","code":"[{\"shape\":\"rect\",\"coords\":\"264,50,277,78\"}]"} {"title":"x and y coordinates at t=0 of the object","description":"Correct!","type":"correct","color":"#FF6600","code":"[{\"shape\":\"rect\",\"coords\":\"90,11,111,34\"},{\"shape\":\"rect\",\"coords\":\"91,59,118,85\"}]"}We can use another equation from Chapter 2 to write down the equations for the projectile’s x and y coordinates x and y at any time t. We let x and y be the projectile’s coordinates at time t=0. Because the x component of acceleration ax is constant, we know that x=x0+v0xt+(1/2)axt2 from Equation 2-10 in Section 2-5. The same equation rewritten for the y direction is y=y0+v0yt+(1/2)ayt2. For projectile motion ax=0 and ay=−g, so these equations become: