
The position of a particle as a function of time is described by relation $x = 3t - 3t^2 + t^3$ where the quantities are expressed in S.I. units. If mass of the particle be 10 kg, the work done in first three seconds is
A. 10 J
B. 30 J
C. 300 J
D. 675 J
Answer
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Hint: We are given position x in terms of another variable t (time), we must differentiate this twice to get the acceleration equation which when multiplied by mass will give us a force equation. Then we can use Force times displacement to get the work done.
Formula used:
For a small displacement dx, caused by a force F the work done is given as:
$W = \int F dx$
Complete step by step answer:
First we write down the expression for position x:
$x = 3t - 3t^2 + t^3$ .
By differentiating this expression twice w.r.t. time we get acceleration as:
$a = \dfrac{d^2 x}{dt^2} = -6 + 6t$.
We can now write the expression for force F = ma; as we know mass of the particle is 10 kg so;
$F = -60 + 60t$
Infinitesimal work done due to this force causing displacement dx can be written as:
$dW = F.dx$
Therefore, we need to determine dx first. From the expression for x, we can write:
$dx = 3 dt - 6t dt + 3t^2 dt$
where we simply differentiate once on both sides of x with respect to time.
Multiply the dx with F first to simplify the integration ahead:
$F.dx = (-60 + 60t).(3 dt - 6t dt + 3t^2 dt)$
$F.dx = -180 dt + 360t dt -180t^2 dt + 180t dt -360t^2 dt + 180t^3 dt$
$F.dx = -180 dt + 540t dt -540t^2 dt + 180t^3 dt$
Performing integration now, we get the work done as:
$W = \int_{0}^{3} (-180 + 540t -540t^2 + 180t^3 )dt$
we kept the limits t = 0 s to t = 3 s.
$W = -180 (t)_{0}^{3}+ 540 \left( \dfrac{t^2}{2} \right)_{0}^{3} -540 \left( \dfrac{t^3}{3} \right)_{0}^{3} + 180 \left( \dfrac{t^4}{4} \right)_{0}^{3} $
$W = -540 + 2430 - 4860 + 3645 = 675 J$
Therefore, the correct answer is option (D). 675 J is the work done in the first 3 seconds.
Note:
The integration in the formula for work usually is done considering the variable to be x (as we had F.dx) but here we made a variable change from x to t with the help of the given expression for x. As we change the variable from x to t we also change the limits accordingly. As we had to find work done for the first 3s, we took initial time t = 0s and final time to be t = 3s in the limits of integral.
Formula used:
For a small displacement dx, caused by a force F the work done is given as:
$W = \int F dx$
Complete step by step answer:
First we write down the expression for position x:
$x = 3t - 3t^2 + t^3$ .
By differentiating this expression twice w.r.t. time we get acceleration as:
$a = \dfrac{d^2 x}{dt^2} = -6 + 6t$.
We can now write the expression for force F = ma; as we know mass of the particle is 10 kg so;
$F = -60 + 60t$
Infinitesimal work done due to this force causing displacement dx can be written as:
$dW = F.dx$
Therefore, we need to determine dx first. From the expression for x, we can write:
$dx = 3 dt - 6t dt + 3t^2 dt$
where we simply differentiate once on both sides of x with respect to time.
Multiply the dx with F first to simplify the integration ahead:
$F.dx = (-60 + 60t).(3 dt - 6t dt + 3t^2 dt)$
$F.dx = -180 dt + 360t dt -180t^2 dt + 180t dt -360t^2 dt + 180t^3 dt$
$F.dx = -180 dt + 540t dt -540t^2 dt + 180t^3 dt$
Performing integration now, we get the work done as:
$W = \int_{0}^{3} (-180 + 540t -540t^2 + 180t^3 )dt$
we kept the limits t = 0 s to t = 3 s.
$W = -180 (t)_{0}^{3}+ 540 \left( \dfrac{t^2}{2} \right)_{0}^{3} -540 \left( \dfrac{t^3}{3} \right)_{0}^{3} + 180 \left( \dfrac{t^4}{4} \right)_{0}^{3} $
$W = -540 + 2430 - 4860 + 3645 = 675 J$
Therefore, the correct answer is option (D). 675 J is the work done in the first 3 seconds.
Note:
The integration in the formula for work usually is done considering the variable to be x (as we had F.dx) but here we made a variable change from x to t with the help of the given expression for x. As we change the variable from x to t we also change the limits accordingly. As we had to find work done for the first 3s, we took initial time t = 0s and final time to be t = 3s in the limits of integral.
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