Examples of integration to get moment of inertia. The moment of inertia in such cases takes the form of a mathematical tensor quantity which requires nine components to completely define it. The concept of moment of inertia for general objects about arbitrary axes is a much more complicated subject. Having called this a general form, it is probably appropriate to point out that it is a general form only for axes which may be called "principal axes", a term which includes all axes of symmetry of objects. Usually, the mass element dm will be expressed in terms of the geometry of the object, so that the integration can be carried out over the object as a whole (for example, over a long uniform rod). The sum over all these mass elements is called an integral over the mass. Note that the differential element of moment of inertia dI must always be defined with respect to a specific rotation axis. This kind of mass element is called a differential element of mass and its moment of inertia is given by Then the moment of inertia contribution by an infinitesmal mass element dm has the same form. Since the moment of inertia of a point mass is defined by Since the moment of inertia of an ordinary object involves a continuous distribution of mass at a continually varying distance from any rotation axis, the calculation of moments of inertia generally involves calculus, the discipline of mathematics which can handle such continuous variables. Where moment of inertia appears in physical quantities The general form of the moment of inertia involves an integral. The moment of inertia of any extended object is built up from that basic definition. The moment of inertia of a point mass with respect to an axis is defined as the product of the mass times the distance from the axis squared. Moment of inertia is defined with respect to a specific rotation axis. That point mass relationship becomes the basis for all other moments of inertia since any object can be built up from a collection of point masses. For a point mass, the moment of inertia is just the mass times the square of perpendicular distance to the rotation axis, I = mr 2. The moment of inertia must be specified with respect to a chosen axis of rotation. It appears in the relationships for the dynamics of rotational motion. Moment of inertia is the name given to rotational inertia, the rotational analog of mass for linear motion. This is called precession, and is analogous to the orbit of a mass under a central force. This changes its direction but not its magnitude, causing the tip of the axle to trace out a circle. If a spinning wheel and axle is supported by one end of the axle, then the torque produced by the weight of the wheel and axle produces a torque that is perpendicular to the angular momentum of the wheel. Acting perpendicular to the velocity, it provides the necessary centripetal force to keep it in a circle. I have included an image of this below: Moreover, in order to obtain the moment of inertia for a thin cylindrical shell (otherwise known as a hoop), we can substitute R1 R2 R, as the shell has a negligible thickness. With the appropriate balance of force, a circular orbit can be produced by a force acting toward the center. By setting R1 0, we can therefore work out the specific moment of inertia equation for a solid cylinder. This is because the product of moment of inertia and angular velocity must remain constant, and halving the radius reduces the moment of inertia by a factor of four. If the string is pulled down so that the radius is half the original radius, then conservation of angular momentum dictates that the ball must have four times the angular velocity. Using a string through a tube, a mass is moved in a horizontal circle with angular velocity ω. HyperPhysics***** Mechanics ***** RotationĬonservation of linear momentum dictates that when a mass strikes an equal mass at rest and sticks to it, the combination must move at half the velocity, because the product of mass and velocity must remain constant. Moment of Inertia Rotational-Linear Parallels More comparisons between linear and angular motion Refer to (Figure) for the moments of inertia for the individual objects. Example 6: When r 1 is 10 m, r 2 is 20 m, and the mass of the annular ring is 14 kg, calculate the moment of inertia of the ring. We have for hollow cylinder, MOI (I) MR 2. In both cases, the moment of inertia of the rod is about an axis at one end. Example 5: If the mass is 10 kg and the radius is 7 m, determine the hollow cylinder’s moment of inertia. In (b), the center of mass of the sphere is located a distance R from the axis of rotation. In (a), the center of mass of the sphere is located at a distance L+R from the axis of rotation. Since we have a compound object in both cases, we can use the parallel-axis theorem to find the moment of inertia about each axis. The radius of the sphere is 20.0 cm and has mass 1.0 kg. The rod has length 0.5 m and mass 2.0 kg. Find the moment of inertia of the rod and solid sphere combination about the two axes as shown below.
0 Comments
Leave a Reply. |
AuthorWrite something about yourself. No need to be fancy, just an overview. ArchivesCategories |