1. A cannon ball M = 10.0kg with V = 2.4×102m/s is broken into 2 parts, if m1 = 6.4kg with

angle 37° and m2 with 53°, what is the magnitude of v1 and v2?

To find the magnitudes of v1 and v2, we can use the principle of conservation of linear momentum. According to this principle, the total momentum before the cannonball breaks apart is equal to the total momentum after the break.

The initial momentum of the cannonball is given by the product of its mass (M) and velocity (V):
p_initial = M * V

After the break, the momentum is split into two parts: p1 and p2.
p1 = m1 * v1
p2 = m2 * v2

Using the principle of conservation of linear momentum, we can write:

p_initial = p1 + p2

Substituting the values given in the question, we have:

M * V = m1 * v1 + m2 * v2

M = 10.0 kg (mass of cannonball)
V = 2.4 × 10^2 m/s (initial velocity)
m1 = 6.4 kg (mass of one part)
m2 = ? (mass of the other part)
v1 = ? (velocity of one part)
v2 = ? (velocity of the other part)

From the given information, we know the mass of one part (m1 = 6.4 kg) and the angle (37°). To find the velocity of this part (v1), we can use the concept of projectile motion.

The horizontal component of the velocity (v1x) remains constant, while the vertical component (v1y) changes due to gravity. We can find v1x and v1y using the following equations:

v1x = v1 * cos(37°)
v1y = v1 * sin(37°)

To find v1, we can use the total initial kinetic energy, which is equal to the sum of the kinetic energies in the horizontal and vertical directions:

1/2 * m1 * (v1x^2 + v1y^2) = 1/2 * M * V^2

Simplifying the equation and substituting the known values, we have:

1/2 * 6.4 * (v1 * cos(37°))^2 + 1/2 * 6.4 * (v1 * sin(37°))^2 = 1/2 * 10.0 * (2.4 × 10^2)^2

Solving this equation will give us the value of v1.

Now, for the second part, we know the angle (53°) but not the mass (m2). Therefore, we cannot directly calculate its velocity (v2) at this point.

If you provide the mass (m2) or any additional information, we can proceed with finding the magnitude of v2 using a similar approach as above.