Question:

A stationary body of mass m explodes into the three parts having masses in the ratio 1:3:3. The two fractions with equal masses move at right angles to each other with a velocity of $ 1.5\,m{{s}^{-1}}. $ The velocity of the third part is:

Updated On: Aug 10, 2024
  • $ 4.5\sqrt{2}\,m{{s}^{-1}} $
  • $ 5\,m{{s}^{-1}} $
  • $ 5\sqrt{32}\,m{{s}^{-1}} $
  • $ 1.5\,m{{s}^{-1}} $
Hide Solution
collegedunia
Verified By Collegedunia

The Correct Option is A

Solution and Explanation

Equate the momenta of the system along two perpendicular axes. Let $ u $ be the velocity and $ \theta $ the direction of the third piece as shown.
Equating the momenta of the system along OA and OB to zero, we get $ 3m\times 1.5-m\times v\cos \theta =0 $ ..(i)
and $ 3m\times 1.5-m\times v\sin \theta =0 $ ..(ii)
These give $ mv=\,\cos \theta =mv\sin \theta $ or $ \cos \theta =\sin \theta $
$ \therefore $ $ \theta ={{45}^{o}} $
Thus, $ \angle AOC=\angle BOC={{180}^{o}}-{{45}^{o}}={{135}^{o}} $
Putting the value of $ \theta $ in E (i), we get $ 4.5\,m=mv\cos {{45}^{o}}=\frac{mv}{\sqrt{2}} $
$ \therefore $ $ v=4.5\sqrt{2}\,m{{s}^{-1}} $
The third piece will go with a velocity of
$ 4.5\sqrt{2}\,m{{s}^{-1}} $
in a direction making an angle of $ {{135}^{o}} $ with either piece.
The square of momentum of third piece is equal to sum of squares of momentum first and second pieces. As from key idea,
$ p_{3}^{2}=p_{1}^{2}+p_{2}^{2} $ or $ {{p}_{3}}=\sqrt{p_{1}^{2}+p_{2}^{2}} $ or $ m{{v}_{3}}=\sqrt{{{(3m\times 1.5)}^{2}}+{{(3m\times 1.5)}^{2}}} $ or $ {{v}_{3}}=4.5\sqrt{2}\,m{{s}^{-1}} $
Was this answer helpful?
1
0

Concepts Used:

Conservation of Energy

In physics and chemistry, the law of conservation of energy states that the total energy of an isolated system remains constant; it is said to be conserved over time.

It also means that energy can neither be created nor destroyed; rather, it can only be transformed or transferred from one form to another. For instance, chemical energy is converted to kinetic energy when a stick of dynamite explodes.

So, mathematically we can represent the law of energy conservation as the following,

The amount of energy spent in a work = The amount of Energy gained in the related work

Now, the derivation of the energy conservation formula is as followed,

Ein − Eout = Δ Esys

We know that the net amount of energy which is transferred in or out of any system is mainly seen in the forms of heat (Q), mass (m) or work (W). Hence, on re-arranging the above equation, we get,

Ein − Eout = Q − W

Now, on dividing all the terms into both the sides of the equation by the mass of the system, the equation represents the law of conservation of energy on a unit mass basis, such as

Q − W = Δ u

Thus, the conservation of energy formula can be written as follows,

Q – W = dU / dt

Here,

Esys = Energy of the system as a whole

Ein = Incoming energy

Eout = Outgoing energy

E = Energy

Q = Heat

M = Mass

W = Work

T = Time