To solve this problem, we must use the principle of conservation of momentum. When the body explodes, the total momentum of the system should remain zero as it was initially at rest.
Let's designate the masses of the three pieces after the explosion as follows:
Since the first two pieces move perpendicular to each other, we can use vector addition to find the resultant momentum that the third piece must balance.
The momentum of the system must be zero, so the momentum of the third piece should be equal and opposite to the vector sum of momenta of the two smaller pieces.
Let's calculate the vector resultant of the momenta of the first two pieces:
The momentum vectors are perpendicular to each other, so we use the Pythagorean Theorem:
p_{\text{net}} = \sqrt{\left(\frac{30M}{4}\right)^2 + \left(\frac{40M}{4}\right)^2}Calculating:
p_{\text{net}} = \sqrt{\frac{900M^2}{16} + \frac{1600M^2}{16}} p_{\text{net}} = \sqrt{\frac{2500M^2}{16}} p_{\text{net}} = \frac{50M}{4} = \frac{25M}{2}The third piece, with a mass of \(m_3 = \frac{M}{2}\), must have a momentum equal and opposite to this, thus:
Solving for \(v_3\), we get:
v_3 = 25 \, \text{m/s}Therefore, the velocity of the third piece is 25 m/s, which matches the correct answer option.
