From the main two kinematic equations describing one-dimensional motion under constant acceleration 1 x = Xo + vot + at? and v = vo + at one can derive other equations that can be useful in solving constant acceleration problems by solving for one term in one equation above and substituting it into the other one to eliminate it. A) Starting from the main two equations eliminate vo to derive x xo = vt- B) Start from the main two equations and eliminate t to derive a(x – xo) = (v² – v,²). 1 — хо) %3D

From the main two kinematic equations describing one-dimensional motion under constant acceleration 1 x = Xo + vot + at? and v = vo + at one can derive other equations that can be useful in solving constant acceleration problems by solving for one term in one equation above and substituting it into the other one to eliminate it. A) Starting from the main two equations eliminate vo to derive x xo = vt- B) Start from the main two equations and eliminate t to derive a(x – xo) = (v² – v,²). 1 — хо) %3D

Name: 3. From the main two kinematic equations describing one-dimensional m
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Description: 3. From the main two kinematic equations describing one-dimensional motion under constantacceleration1x = xo + vot +, atandv = vo + atone can derive other equations that can be useful in solving constant acceleration problems bysolving for one term

College Physics

11th Edition

ISBN:9781305952300

Author:Raymond A. Serway, Chris Vuille

Publisher:Raymond A. Serway, Chris Vuille

Chapter2: Motion In One Dimension

Section: Chapter Questions

Problem 42P: The kinematic equations can describe phenomena other than motion through space and time. Suppose x...

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