In this question, you will be asked to work on mechanical vibration in a system made of a circular disk attached at the end of a shaft, both shaft and disk inside a medium providing a damping proportional to the angular velocity. The system can be modeled based on a mass-spring and damper system. This system can be useful as a first introduction to either rotating shaft in water (propeller), or as to model part of a rotating shaft in oil. Of course, the model described here is merely the introduction. Mass M ↑ L Shaft R Important concept to consider: Moment of inertia: The moment of inertia can be understood as the inertia of the rotating body, or the physical phenomena that prevent the motion (for example, the inertia in a linear motion is the mass of the object; for rotation, the geometry of the object is also important). It will be represented by the letter I, and you will have to work with the moment of inertia about the central axis of the rotation. Shear modulus: In the current application, it is the pressure needed to produce an elastic displacement along the plane perpendicular to the axis of rotation. We will use the letter G to represent it and it will be a constant. Polar surface moment of inertia: This is a geometric value based on the cross section of the shaft. The symbol used will be J. The global motion of the object will be described using the angular position 0. The general equation you will consider to start your study will be Newton's second law in angular motion, thus ΣΜ = 16 M Where represent the torque applied on the shaft. For the system at hand, consider the mass (disk) attached to a vertical shaft that fix at the top end and free to rotate along the vertical z axis. The mass is in a liquid that impart a damping that is 4 times the angular velocity of rotation. To describe the system, you can use the following data: Shaft: L = 0.5 m, r = 0.01 m G = 79.6 GPa πρ J is the polar moment of inertia of the shaft (cross-section) - use shaft 2 r is the radius of the Mass: Radius: R = 0.5 m, thickness: 0.2 m, density: 5000 kg/m^3 I is moment of inertia about the center, use ¹¹mR² Angular motion: Use the angle position (t) to describe the motion, with and Ꮎ Elastic torque: Damping torque: -40 a) Start with Newton's second law for rotation to build a differential equation describing the system at hand. b) Find the general solution of the system c) Find the particular solution if at time 0, the initial angle is π/6 and the initial angular velocity is 0. d) Assuming you change the mass by a sphere with the same radius and density, and that the damping torque is now -3ė, find the difference in the frequency of oscillation between this scenario and the one studied before? (you will need to find the mass moment of inertia of the sphere)

In this question, you will be asked to work on mechanical vibration in a system made of a circular disk attached at the end of a shaft, both shaft and disk inside a medium providing a damping proportional to the angular velocity. The system can be modeled based on a mass-spring and damper system. This system can be useful as a first introduction to either rotating shaft in water (propeller), or as to model part of a rotating shaft in oil. Of course, the model described here is merely the introduction. Mass M ↑ L Shaft R Important concept to consider: Moment of inertia: The moment of inertia can be understood as the inertia of the rotating body, or the physical phenomena that prevent the motion (for example, the inertia in a linear motion is the mass of the object; for rotation, the geometry of the object is also important). It will be represented by the letter I, and you will have to work with the moment of inertia about the central axis of the rotation. Shear modulus: In the current application, it is the pressure needed to produce an elastic displacement along the plane perpendicular to the axis of rotation. We will use the letter G to represent it and it will be a constant. Polar surface moment of inertia: This is a geometric value based on the cross section of the shaft. The symbol used will be J. The global motion of the object will be described using the angular position 0. The general equation you will consider to start your study will be Newton's second law in angular motion, thus ΣΜ = 16 M Where represent the torque applied on the shaft. For the system at hand, consider the mass (disk) attached to a vertical shaft that fix at the top end and free to rotate along the vertical z axis. The mass is in a liquid that impart a damping that is 4 times the angular velocity of rotation. To describe the system, you can use the following data: Shaft: L = 0.5 m, r = 0.01 m G = 79.6 GPa πρ J is the polar moment of inertia of the shaft (cross-section) - use shaft 2 r is the radius of the Mass: Radius: R = 0.5 m, thickness: 0.2 m, density: 5000 kg/m^3 I is moment of inertia about the center, use ¹¹mR² Angular motion: Use the angle position (t) to describe the motion, with and Ꮎ Elastic torque: Damping torque: -40 a) Start with Newton's second law for rotation to build a differential equation describing the system at hand. b) Find the general solution of the system c) Find the particular solution if at time 0, the initial angle is π/6 and the initial angular velocity is 0. d) Assuming you change the mass by a sphere with the same radius and density, and that the damping torque is now -3ė, find the difference in the frequency of oscillation between this scenario and the one studied before? (you will need to find the mass moment of inertia of the sphere)

Trigonometry (MindTap Course List)

8th Edition

ISBN:9781305652224

Author:Charles P. McKeague, Mark D. Turner

Publisher:Charles P. McKeague, Mark D. Turner

Chapter8: Complex Numbers And Polarcoordinates

Section: Chapter Questions

Problem 8CLT

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