a particle moves in a straight line in such a manner that s=1/2vt, s being the distance travelled in time t and v the velocity at the end of time t. prove that the acceleration is constant
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motion in a single direction.
s = v t / 2
velocity = ds / dt
v = 1/2 [ v * 1 + t dv/dt ]
v = 1/2 [ v + a t ]
1/2 v = 1/2 at
v = a t
acceleration a = dv/dt = a * 1 + t * d a / dt
a = a + t * da/dt
=> da / dt = 0
=> a = dv/dt = acceleration = constant.
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we can perhaps do the following way:
if acceleration is constant then, the equations of motion are:
v = u + at
s = u t + 1/2 a t²
v² - u² = 2 a s
in our context, s = 1/2 v t
v = 2 s / t, differentiate wrt time t:
a = dv/dt
= 2 [t * ds/dt - s * 1 ] / t²
= 2 [ v t - s ] / t²
= 2 [ v t - 1/2 vt ] / t²
= 2 * vt/2 /t²
= v / t
da/dt = [ t * dv/dt - v * 1 ] /t²
= [ t * a - v ] / t²
= 0 as v = a t
Hence, Acceleration is constant. as its derivative is zero.
s = v t / 2
velocity = ds / dt
v = 1/2 [ v * 1 + t dv/dt ]
v = 1/2 [ v + a t ]
1/2 v = 1/2 at
v = a t
acceleration a = dv/dt = a * 1 + t * d a / dt
a = a + t * da/dt
=> da / dt = 0
=> a = dv/dt = acceleration = constant.
====================================
we can perhaps do the following way:
if acceleration is constant then, the equations of motion are:
v = u + at
s = u t + 1/2 a t²
v² - u² = 2 a s
in our context, s = 1/2 v t
v = 2 s / t, differentiate wrt time t:
a = dv/dt
= 2 [t * ds/dt - s * 1 ] / t²
= 2 [ v t - s ] / t²
= 2 [ v t - 1/2 vt ] / t²
= 2 * vt/2 /t²
= v / t
da/dt = [ t * dv/dt - v * 1 ] /t²
= [ t * a - v ] / t²
= 0 as v = a t
Hence, Acceleration is constant. as its derivative is zero.
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