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Question: A particle moves in a straight line, according to the law \[x=4a[t+a\sin (\dfrac{t}{a})]\], where \[...

A particle moves in a straight line, according to the law x=4a[t+asin(ta)]x=4a[t+a\sin (\dfrac{t}{a})], where xx is its position in meters, tt in sec. & aa is some constants, then velocity is zero at
A) x=4a2πmetersx=4{{a}^{2}}\pi meters
B) t=πsec.t=\pi \sec .
C) t=0sec.t=0\sec .
D) nonenone

Explanation

Solution

Velocity is the rate of change of displacement. To get velocity the equation of displacement must be differentiated with respect to time. Then solve as per the given question.

Complete step by step answer:
The given equation is for displacement and we are required to find the time when velocity is zero.
Since velocity is the rate of change of displacement hence we will differentiate the given equation.
x=4a[t+asin(ta)]\Rightarrow x=4a[t+a\sin (\dfrac{t}{a})]
Here xx is the displacement
aa is a constant
tt is the time in seconds

Let’s first simplify this equation,
x=4at+4a2sin(ta)\Rightarrow x=4at+4{{a}^{2}}\sin (\dfrac{t}{a})
Now differentiating this equation with respect to time we will get equation of velocity since v=dxdtv=\dfrac{dx}{dt}
dxdt=4a+4a2(cos(ta))(1a)\Rightarrow \dfrac{dx}{dt}=4a+4{{a}^{2}}(\cos (\dfrac{t}{a}))(\dfrac{1}{a})
Here d(4at)dt=4a\dfrac{d(4at)}{dt}=4a since aa is constant as given in the question.
And it is also known from basic differentiation rules that d(sinθ)dθ=cosθ\dfrac{d(\sin \theta )}{d\theta }=\cos \theta
Also d(sinaθ)dθ=(cosaθ)(daθdθ)\dfrac{d(\sin a\theta )}{d\theta }=(\cos a\theta )(\dfrac{da\theta }{d\theta })
We finally get
v=dxdt=4a+4acos(ta)\Rightarrow v=\dfrac{dx}{dt}=4a+4a\cos (\dfrac{t}{a})
That is equation of velocity is given as
v=4a+4acos(ta)\Rightarrow v=4a+4a\cos (\dfrac{t}{a})
We need to calculate time for which the velocity is zero, hence we will put v=0v=0 in the above equation
0=4a+4acos(ta)\Rightarrow 0=4a+4a\cos (\dfrac{t}{a})
On solving further we get,
0=4a[1+costa)]\Rightarrow 0=4a[1+\cos \dfrac{t}{a})]
0=1+cos(ta)\Rightarrow 0=1+\cos (\dfrac{t}{a})
1=cos(ta)\Rightarrow -1=\cos (\dfrac{t}{a})
Now this equation is of the form, cosθ=1\cos \theta =-1
We need to find θ\theta such that cosθ=1\cos \theta =-1, let’s check the graph of cosθ\cos \theta
The value of cosθ\cos \theta is equal to 1-1 when the value of θ\theta is π\pi .
Therefore, cos(ta)=1\cos (\dfrac{t}{a})=-1
ta=π\Rightarrow \dfrac{t}{a}=\pi
t=aπ\Rightarrow t=a\pi
Therefore the velocity is zero at t=aπt=a\pi which is not given in the option.
Hence the correct option is (D)(D) none of these

Note: If we again differentiate the equation of velocity with respect to time, we will get an equation for acceleration. Do remember that there can be infinitely many solutions as the graph of cosθ\cos \theta is periodic in nature. It repeats after an interval of 2π2\pi . This implies that the velocity will again be zero for t=πa+2πat=\pi a+2\pi a, t=πa+4πat=\pi a+4\pi a and so on.