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Question: The position of a particle moving along the \( X \) -axis is expressed as \( x = a{t^3} + b{t^2} + c...

The position of a particle moving along the XX -axis is expressed as x=at3+bt2+ct+dx = a{t^3} + b{t^2} + ct + d .The initial acceleration of the particle is
(A) 6a6a
(B) 2b2b
(C) a+ba + b
(D) a+ca + c

Explanation

Solution

Use the formula of instantaneous acceleration of a particle at a time tt . The instantaneous acceleration of a particle is given by, a=dvdt=d2xdt2a = \dfrac{{dv}}{{dt}} = \dfrac{{{d^2}x}}{{d{t^2}}} .

Complete answer:
We have here, the expression of the position or displacement at a time tt is x=at3+bt2+ct+dx = a{t^3} + b{t^2} + ct + d .Now to find the acceleration of the particle for a particular time we first have to differentiate this equation with respect to tt , as tt is here the independent variable and xx is dependant on tt .
Now, to differentiate this expression of position, we have to use the formula for differentiation and use it twice two find the expression of acceleration at a particular time tt .
The formula for differentiation of xn{x^n} with respect to xx is, ddxxn=nx(n1)\dfrac{d}{{dx}}{x^n} = n{x^{\left( {n - 1} \right)}} .
So, let's find the differentiation of xx with respect to tt here.
Upon doing that, we first get the expression for velocity as,
v=ddt(x)=ddtat3+dvdtbt2+dvdtct+dvdtdv = \dfrac{d}{{dt}}(x) = \dfrac{d}{{dt}}a{t^3} + \dfrac{{dv}}{{dt}}b{t^2} + \dfrac{{dv}}{{dt}}ct + \dfrac{{dv}}{{dt}}d
=addtt3+bdvdtt2+cdvdtt= a\dfrac{d}{{dt}}{t^3} + b\dfrac{{dv}}{{dt}}{t^2} + c\dfrac{{dv}}{{dt}}t
Since, differentiation of ddxCf(x)=Cddxf(x)\dfrac{d}{{dx}}Cf(x) = C\dfrac{d}{{dx}}f(x) where CC is any constant
Now, using the formula we get,
=3at(31)+2bt(21)+1ct(11)= 3a{t^{\left( {3 - 1} \right)}} + 2b{t^{\left( {2 - 1} \right)}} + 1c{t^{\left( {1 - 1} \right)}}
On simplifying which becomes,
=3at2+2bt1+1ct0= 3a{t^2} + 2b{t^1} + 1c{t^0}
=3at2+2bt+c= 3a{t^2} + 2bt+ c [Since, t0=1{t^0} = 1 ]
Now on differentiating this expression again we get the expression for acceleration of the particle at an instant of time.
So, differentiating vv we get the acceleration α\alpha as ,
α=dvdt=d2xdt2=ddt(3at2+2bt+c)\alpha = \dfrac{{dv}}{{dt}} = \dfrac{{{d^2}x}}{{d{t^2}}} = \dfrac{d}{{dt}}(3a{t^2} + 2bt + c)
Simplifying we get,
=ddt(3at2)+ddt(2bt)+ddt(c)= \dfrac{d}{{dt}}(3a{t^2}) + \dfrac{d}{{dt}}(2bt) + \dfrac{d}{{dt}}(c)
=3addtt2+(2bddtt)+ddt(c)= 3a\dfrac{d}{{dt}}{t^2} + (2b\dfrac{d}{{dt}}t) + \dfrac{d}{{dt}}(c)
Therefore it becomes,
=32at21+2bt11+0= 3 \cdot 2a{t^{2 - 1}} + 2 \cdot b{t^{1 - 1}} + 0
Since, differentiation of a constant is zero, ddxC=0\dfrac{d}{{dx}}C = 0
Thus, acceleration of the particle at a instant of time tt is,
α=6at+2b\alpha = 6at + 2b .
Now, here we have been given to find the initial acceleration of the particle, for that condition time tt of the particle is zero.
Therefore, putting the value of time in the expression of the derived acceleration we get,
α=6a0+2b\alpha = 6a \cdot 0 + 2b .
Which becomes,
α=2b\alpha = 2b .
Therefore, the initial acceleration of the particle is 2b2b .
Hence option (B) is correct.

Note:
The acceleration of a particle is generally defined as velocity per time which is v2v1t2t1=ΔvΔt\dfrac{{{v_2} - {v_1}}}{{{t_2} - {t_1}}} = \dfrac{{\Delta v}}{{\Delta t}} . Whereas the instantaneous acceleration of the particle is when the time difference tends to zero that means limΔt0Δt\mathop {\lim }\limits_{\Delta t \to 0} \Delta t .