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DRB Urm PDF

Uniform rectilinear motion involves constant velocity and zero acceleration. The position (x) is equal to the initial position (x0) plus the velocity (v) multiplied by time (t). Uniformly accelerated rectilinear motion involves constant acceleration. The velocity (v) is equal to the initial velocity (v0) plus the acceleration (a) multiplied by time (t). The position (x) is equal to the initial position (x0) plus the initial velocity (v0) multiplied by time (t) plus half the acceleration (a) multiplied by time (t) squared. The final velocity (v) can be determined from the initial velocity (v0) and the acceleration (a) using the equation

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177 views1 page

DRB Urm PDF

Uniform rectilinear motion involves constant velocity and zero acceleration. The position (x) is equal to the initial position (x0) plus the velocity (v) multiplied by time (t). Uniformly accelerated rectilinear motion involves constant acceleration. The velocity (v) is equal to the initial velocity (v0) plus the acceleration (a) multiplied by time (t). The position (x) is equal to the initial position (x0) plus the initial velocity (v0) multiplied by time (t) plus half the acceleration (a) multiplied by time (t) squared. The final velocity (v) can be determined from the initial velocity (v0) and the acceleration (a) using the equation

Uploaded by

Shang Divina Ebrada
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
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Download as PDF, TXT or read online on Scribd
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28/01/2019

Uniform Rectilinear Motion Uniformly Accelerated Rectilinear Motion


For particle in uniformly accelerated rectilinear motion, the acceleration of
For particle in uniform rectilinear motion, the acceleration is zero and
the particle is constant.
the velocity is constant.
v t
dv
dx  a  constant  dv  a  dt v  v0  at
 v  constant dt v0 0
dt
x t v  v0  at
 dx  v  dt
x0 0 x t
dx
x  x0  vt dt
 v0  at  dx   v0  at dt x  x0  v0t  12 at 2
x0 0
x  x0  vt
x x0  v0t  12 at 2

v 2  v02   ax  x0 
v x
dv
v  a  constant  v dv  a  dx 1
2
dx v0 x0

v 2  v02  2a x  x0 
11 - 1 11 - 2

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