A bicycle wheel is mounted on a fixed, frictionless axle, with a light string wound around its rim. The wheel has moment of inertia I=kmr2I=kmr2, where mm is its mass, rr is its radius, and kk is a dimensionless constant between zero and one. The wheel is rotating counterclockwise with angular speed ω0ω0 t=0t=0 someone starts pulling the string with a force of magnitude FF A. Suppose that after a certain time tLtL LL ωfinalωfinal of the wheel? Express your answer in terms of LL FF II ω0ω0 B. What is the instantaneous power PP delivered to the wheel via the force F⃗F→ at time t=0t=0? Express the power in terms of some or all of the variables given in the problem introduction.
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.
A bicycle wheel is mounted on a fixed, frictionless axle, with a light string wound around its rim. The wheel has moment of inertia I=kmr2I=kmr2, where mm is its mass, rr is its radius, and kk is a dimensionless constant between zero and one. The wheel is rotating counterclockwise with angular speed ω0ω0 t=0t=0 someone starts pulling the string with a force of magnitude FF
A. Suppose that after a certain time tLtL LL ωfinalωfinal of the wheel?
Trending now
This is a popular solution!
Step by step
Solved in 3 steps with 3 images
