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| Case of Uniform Acceleration |
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| We know that |
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When a particle moves with uniform motion in a straight line in the
given plane, the above equation always yields the same value of ,
whatever may be the values of t and t'. However, when a particle
moves in a plane with uniform acceleration,
begins to depend on t and t'. This is because of change in velocity with time. |
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In the case of uniformly accelerated motion in a plane, we can still retain equation (1) but with a slight modification. Instead of velocity ,
we define another vector called average velocity vector. It is denoted by and is given by, |
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This equation refers to an 'interval of time' and not to an instant of
time. However, there exists a velocity vector (t)
at each instant of time just as there exists a position vector
at each time t. |
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| A particle is said to move with uniform acceleration if its velocity changes by equal amounts in equal intervals of time, however small these intervals may be. |
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Acceleration is the rate of the change in velocity to the corresponding
time interval. It is denoted by and is given by |
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As in the case of uniform velocity, the
above equation will yield the same value of ,
whatever may be the values of t' and t. The manner of variation
of velocity vector with time is given by the following equations.\ |
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Next, consider how the position vector
changes with time in the case of uniformly accelerated motion. |
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The average velocity in the time interval from t to is given by |
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| The displacement undergone in the time interval from t to tl is given by |
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| Substituting for Vav from equation (2) in the above equation we have, |
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| This equation relates two different positions of a particle moving with uniform acceleration in a plane. |
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| If we replace t' by t and t by 0, |
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| In terms of rectangular components, |
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| Each of these equations, when considered separately, represents uniformly accelerated motion in one dimension. |
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In equation (3), are
the position and velocity vectors respectively at t = 0.
is the acceleration vector which is supposed to be constant. |
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In general, the vectors and
are not in the same direction. |
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Therefore, in order to find the sum of the three terms, the laws of
vector addition will have to be used. The vector
t is in the same direction as
itself but, its magnitude increases linearly with time.
The vector is in the direction of .
Its magnitude varies as the
square of the time. |
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| The figure below represents the following equation |
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Thus, we see that the velocity at any time t is the vector sum of the
velocity at t = 0 and the additional velocity acquired by
the particle in time t due to uniform acceleration .
Moreover, the same equation
can also be expressed in the following two component forms, viz. |
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