
The relation between time $t$ and distance $x$ is $ t = \alpha {x^2} + \beta x $ where $ \alpha $ and $ \beta $ are constants.Find out the relation between acceleration and velocity.
(A) $ v^3 $
(B) $ v^2 $
(C) $ v^{3/2} $
(D) $ v^{2/3} $
Answer
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Hint
We will differentiate the equation twice. According to Newton's second law when a constant force acts on a massive body, it causes it to accelerate, i.e., to change its velocity, at a constant rate. In the simplest case, a force applied to an object at rest causes it to accelerate in the direction of the force.
Complete step by step answer
As we know the derivative form of acceleration= change of velocity with respect to time
$ \Rightarrow a = \dfrac{{dv}}{{dt}} $
Derivative form of velocity = change of position with respect to tame $ \Rightarrow v = \dfrac{{dx}}{{dt}} $ ......[where x is displacement]
$ t = \alpha {x^2} + \beta x $
Now differentiate the equation with respect to t
$ \Rightarrow \dfrac{d}{{dt}}(t) = \alpha 2x\dfrac{{dx}}{{dt}} + \beta \dfrac{{dx}}{{dt}} $
$ \Rightarrow 1 = 2\alpha x + \beta (\dfrac{{dx}}{{dt}}) $ ..........equation 1
We know $ \dfrac{{dx}}{{dt}} = v $ ,putting the value of equation 1
$ \Rightarrow 1 = (2\alpha x + \beta )v $
$ \Rightarrow \dfrac{1}{v} = 2\alpha x + \beta $
Again differentiate the equation with respect to t
$ \Rightarrow \dfrac{d}{{dt}}\dfrac{1}{v} = \dfrac{d}{{dt}}2\alpha x + \dfrac{d}{{dt}}\beta $
$ \Rightarrow - \dfrac{1}{{{v^2}}}\dfrac{{dv}}{{dt}} = 2\alpha \dfrac{{dx}}{{dt}} $
We know that $ \dfrac{{dv}}{{dt}} = a $ ,putting the value in the equation
$- \dfrac{1}{{{v^2}}}a = 2\alpha v $
$a = - 2\alpha {v^3} $
$a \propto {v^3} $ … [where -2 $ \alpha $ is constant]
Option (A) is the correct answer.
Note
Velocity is the derivative of position with respect to time: $v=\dfrac{dx}{dt}$.
Acceleration is the derivative of velocity with respect to time: $a=\dfrac{dv}{dt}=\dfrac{d^2{x}}{dt^2}$.
We will differentiate the equation twice. According to Newton's second law when a constant force acts on a massive body, it causes it to accelerate, i.e., to change its velocity, at a constant rate. In the simplest case, a force applied to an object at rest causes it to accelerate in the direction of the force.
Complete step by step answer
As we know the derivative form of acceleration= change of velocity with respect to time
$ \Rightarrow a = \dfrac{{dv}}{{dt}} $
Derivative form of velocity = change of position with respect to tame $ \Rightarrow v = \dfrac{{dx}}{{dt}} $ ......[where x is displacement]
$ t = \alpha {x^2} + \beta x $
Now differentiate the equation with respect to t
$ \Rightarrow \dfrac{d}{{dt}}(t) = \alpha 2x\dfrac{{dx}}{{dt}} + \beta \dfrac{{dx}}{{dt}} $
$ \Rightarrow 1 = 2\alpha x + \beta (\dfrac{{dx}}{{dt}}) $ ..........equation 1
We know $ \dfrac{{dx}}{{dt}} = v $ ,putting the value of equation 1
$ \Rightarrow 1 = (2\alpha x + \beta )v $
$ \Rightarrow \dfrac{1}{v} = 2\alpha x + \beta $
Again differentiate the equation with respect to t
$ \Rightarrow \dfrac{d}{{dt}}\dfrac{1}{v} = \dfrac{d}{{dt}}2\alpha x + \dfrac{d}{{dt}}\beta $
$ \Rightarrow - \dfrac{1}{{{v^2}}}\dfrac{{dv}}{{dt}} = 2\alpha \dfrac{{dx}}{{dt}} $
We know that $ \dfrac{{dv}}{{dt}} = a $ ,putting the value in the equation
$- \dfrac{1}{{{v^2}}}a = 2\alpha v $
$a = - 2\alpha {v^3} $
$a \propto {v^3} $ … [where -2 $ \alpha $ is constant]
Option (A) is the correct answer.
Note
Velocity is the derivative of position with respect to time: $v=\dfrac{dx}{dt}$.
Acceleration is the derivative of velocity with respect to time: $a=\dfrac{dv}{dt}=\dfrac{d^2{x}}{dt^2}$.
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