Physics, asked by ceomikeman, 10 months ago

can anyone explain? ​

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Answers

Answered by Anonymous
16

SOLUTION

Let 't1' be the time for which it accelerates, 'v' be the velocity after his tome. Now,when the acceleration is alpha.

 =  >v = 0  +  \alpha t1 \\  =  > v =  \alpha t1 \\  =  > t1 =  \frac{v}{ \alpha }

Then it decelerates at rate Beta & stops at t2.

so,

0 = v -  \beta t2 \\  =  > v =  \beta t2 \\  =  > t2 =  \frac{v}{ \beta }

Now,

t = t1   + t2 = ( \frac{v}{ \alpha } )  + ( \frac{ v}{ \beta } ) = v( \frac{ \alpha  +  \beta }{ \alpha  \beta } ) \\  \\  =  > v = t( \frac{ \alpha  \beta }{ \alpha  +  \beta } )

Now,

Distance travelled in time t1 is found as,

 {v}^{2}  =  {0}^{2}  + 2 \alpha s1 \\  =  > s1 =  \frac{ {v}^{2} }{2 \alpha }

Distance travelled in time t2 is found as,

 {0}^{2}  =  {v}^{2}  - 2 \beta s2 \\  =  > s2 =  \frac{ {v}^{2} }{2 \beta }

Total distance travelled is:

S= s1+ s2

=) S= v^2 (2alpha)+ v^2 /(2beta)

=)S= [v^2/2 ] [(1/alpha+ 1/beta]

=)S= [v^2/2] [(alpha+beta)/alpha.beta]

=)S= 1/2[t[alpha.beta/alpha+beta]]^2 [(alpha + beta)/alpha.beta]

=)S= 1/2t[alpha.beta/(Alpha+beta)]

hope it helps ☺️⬆️

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