Physics, asked by ShivamKashyap08, 11 months ago

For a particle moving along a straight line and its position X is given by {X  = 2 {e}^{ - 2t}} the way it is t is time . Relation between velocity v and acceleration a is given by
1. a = - v
2.a = v
3.a = - 2v
4.a = 2v

Only correct answers accepted ​

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Answers

Answered by Anonymous
32

Answer:

(3) a = -2v

Explanation:

It is being given that, position of the particle in straight line varies by Following equation :-

{X = 2 {e}^{ - 2t}}

We know that, On differentiation of position wrt time, we get velocity as a function of time.

So , differentiate the Following equation :-

We get ,

 \frac{dx}{dt}  = 2 \frac{d( {e}^{ - 2t})}{dt}   = 2 \times  {e}^{ - 2t}  \times  - 2 =  - 4 {e}^{ - 2t}

Now, dx/dt = velocity

 =  > v =  - 4 {e}^{ - 2t}

..................(i)

Now, again differentiate the velocity equation wrt time,

we get,

 =  >  \frac{dv}{dt}  =  - 4 \times  {e}^{ - 2t}  \times  - 2

So, acceleration is

 =  > a = 8 {e}^{ - 2t}

...................(ii)

on comparing equation (i) and (ii), we get

 =  > a =  - 2v

Hence, option (3) is correct.

Answered by Anonymous
15

\Huge{\underline{\underline{\mathfrak{Question \ \colon }}}}

For a particle moving along a straight line and its position X is given by {X = 2 {e}^{ - 2t}} the way it is t is time . Relation between velocity v and acceleration a is given by

1) a = - v

2) a = v

3)a = - 2v

4)a = 2v

\Huge{\underline{\underline{\mathfrak{Answer \ \colon }}}}

From the Question,

The position vector of the particle is defined by the relation :

 \large{ \tt{x = 2 {e}^{ - 2t} }} \\

\rule{300}{2}

To find

Relation between velocity and acceleration of the particle

\rule{300}{2}

Differentiating x w.r.t t,we get velocity of the particle :

 \sf{v =  \frac{dx}{dt} } \\  \\  \leadsto \:  \sf{v =  \frac{d(2 {e}^{ - 2t)} }{dt} } \\  \\  \huge{ \leadsto \:  \boxed{ \boxed{ \tt{ \green{v =  - 4 {e}^{ - 2t} \: m {s}^{ - 1}  }}}}}

\rule{300}{2}

Differentiating v w.r.t to t,we get acceleration of the particle :

 \sf{a =  \frac{dv}{dt} } \\  \\  \leadsto \:  \sf{a =  \frac{d( - 4 {e}^{ - 2t}) }{dt} } \\  \\  \huge{ \leadsto \:  \boxed{ \boxed{ \tt{ \green{a = 8 {e}^{ - 2t} \: m {s}^{ - 2}  }}}}}

\rule{300}{2}

\rule{300}{2}

Dividing values of acceleration and velocity,we get :

 \sf{ \frac{a}{v}  =  -  \frac{8 \cancel{ {e}^{ - 2t}} }{4 \cancel{ {e}^{ - 2t} }} } \\  \\  \huge{ \leadsto \:  \sf{a =  - 2v}}

\rule{300}{2}

\rule{300}{2}

Third Option is correct

\rule{300}{2}

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