A spherical satellite of approximately uniform density with radius 5.7 m and mass 240 kg is originally moving with v (2600, 0, 0) m/s, and is originally rotating with an angular speed 2 rad/s, in the direction shown in the diagram. A s junk of mass 8.0 kg is initially moving toward the satellite with velocity ( – 2200, 0, 0) m/s. The space junk hits the lite as c wn in the fcure belew and movOs off with Ooloritu ( 1300 180. 0\ mle Reth befere and
Angular Momentum
The momentum of an object is given by multiplying its mass and velocity. Momentum is a property of any object that moves with mass. The only difference between angular momentum and linear momentum is that angular momentum deals with moving or spinning objects. A moving particle's linear momentum can be thought of as a measure of its linear motion. The force is proportional to the rate of change of linear momentum. Angular momentum is always directly proportional to mass. In rotational motion, the concept of angular momentum is often used. Since it is a conserved quantity—the total angular momentum of a closed system remains constant—it is a significant quantity in physics. To understand the concept of angular momentum first we need to understand a rigid body and its movement, a position vector that is used to specify the position of particles in space. A rigid body possesses motion it may be linear or rotational. Rotational motion plays important role in angular momentum.
Moment of a Force
The idea of moments is an important concept in physics. It arises from the fact that distance often plays an important part in the interaction of, or in determining the impact of forces on bodies. Moments are often described by their order [first, second, or higher order] based on the power to which the distance has to be raised to understand the phenomenon. Of particular note are the second-order moment of mass (Moment of Inertia) and moments of force.
 alt="A spherical satellite of approximately uniform density with radius 5.7 m and mass 240 kg is originally moving with velocity
(2600, 0, 0) ms, and is originally rotating with an angular speed 2 rad/s, in the direction shown in the diagram. A small piece of space
junk of mass 8.0 kg is initially moving toward the satellite with velocity ( - 2200, 0, 0) m/s. The space junk hits the edge of the
satellite as shown in the figure below, and moves off with a new velocity ( – 1300, 480, 0) m/s. Both before and after the collision,
the rotation of the space junk is negligible.
V3
m
M, R, I
Part 1
(a) Just after the collision, what are the components of the center-of-mass velocity of the satellite (vy and vy) and its rotational
speed w? (For Vx, enter your answer to at least four significant figures.)
Vy =
i
m/s
Vy =
i
m/s
i
rad/s
Part 2
(b) Calculate the rise in the internal energy of the satellite and space junk combined.
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