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Question: A particle of mass \(4\;m\) is projected from the ground at some angle with the horizontal. Its hori...

A particle of mass 4  m4\;m is projected from the ground at some angle with the horizontal. Its horizontal range is RR. At the highest point its path breaks into two pieces of masses mm and 3  m3\;m respectively, such that the smaller mass comes to rest. The larger mass finally falls at a distance xx from the point of projection, where xx is equal to:
A. 2R3\dfrac{2R}{3}
B. 7R6\dfrac{7R}{6}
C. 5R4\dfrac{5R}{4}
D. none of these

Explanation

Solution

A body when projected at an inclination from the ground, I said to experience projectile motion. Then the path followed by the body is called the ballistic trajectory, which is a curved parabolic path. Here, we need to calculate the distance covered by the body after breaking into two pieces.
Formula used:
mv=constantmv=constant
v=xtv=\dfrac{x}{t}

Complete answer:
Let uu be the initial velocity of the body which is projected at an angle θ\theta from the horizontal. Then the initial velocity uu can be resolved into two components along the x and y axis respectively .Let HH and RR be the maximum distances along the x and y-axis respectively, during the time of flight TT Consider the figure as shown below:

We know that the distance covered by the body along the x and y-axis respectively is given as, RR and HH which is the maximum horizontal range and maximum height attained by the object.
Then , we have R=2ucosθtR=2ucos \theta t
The maximum height HH is attained at R2\dfrac{R}{2}
Here, the 4  m4\;m body breaks at HH into 3  m3\;m and mm. Also, after breaking the velocity of the mm particle becomes 00. And let the velocity of the 3  m3\;m be vv.
From the conservation of momentum, we can say that the momentum of the body before breaking is equal to the sum of the momentum of the particles after braking.
    4mucosθ=3mv+m0\implies 4mucos\theta=3mv+m0
    v=43ucosθ\implies v=\dfrac{4}{3}ucos\theta
Let the distance covered by the 3  m3\;m body be xx in time tt, then we have, x=vtx=vt
    x=43ucosθt\implies x=\dfrac{4}{3}ucos\theta t
Replacing ucosθtucos\theta t as R2\dfrac{R}{2}, we get
    x=43×R2\implies x=\dfrac{4}{3}\times \dfrac{R}{2}
    x=4R6\implies x=\dfrac{4R}{6}
Then the total distance covered by the body is given as D=R2+xD=\dfrac{R}{2}+x
    D=R2(1+43)\implies D=\dfrac{R}{2}\left(1+\dfrac{4}{3}\right)
    D=7R6\implies D=\dfrac{7R}{6}

Thus the correct answer is option B. 7R6\dfrac{7R}{6}

Note:
When the object is on the air, the only force acting on it is the force due to gravity, which pulls the object back to the surface at the speed of acceleration due to gravity. Note that the range of the projected body is generally greater than the distance covered by it when dropped from the same height.