Cheyanne Rimer, Jeremy Massari, William Ortiz, Jordan Cooper, and Duncan Godsey Rotational Mechanics.

Slides:



Advertisements
Similar presentations
Angular Quantities Correspondence between linear and rotational quantities:
Advertisements

Rotational Mechanics Ch. 11.
Angular Momentum The vector angular momentum of the point mass m about the point P is given by: The position vector of the mass m relative to the point.
Rotational Motion Chapter Opener. Caption: You too can experience rapid rotation—if your stomach can take the high angular velocity and centripetal acceleration.
Chapter 9 Rotational Dynamics.
Ch 9. Rotational Dynamics In pure translational motion, all points on an object travel on parallel paths. The most general motion is a combination of translation.
Physics Montwood High School R. Casao
Rotational Motion.
Rotational Motion October 31, 2005 and November 2, 2005.
Rigid body rotations inertia. Constant angular acceleration.
Dynamics of Rotational Motion
Warm Up Ch. 9 & 10 1.What is the relationship between period and frequency? (define and include formulas) 2.If an object rotates at 0.5 Hz. What is the.
Rotational Inertia and Angular Momentum. Inertia The resistance of an object to change its state of motion Depends on mass (the bigger the mass, the bigger.
Rotational Mechanics.
Rotational Motion - refers to motion of a body about a fixed axis of rotation wherein, the particles have the same instantaneous angular velocity.
Chapter 11 Rotational Mechanics. Torque If you want to make an object move, apply a force. If you want to make an object rotate, apply a torque. Torque.
Chapter 11 Rotational Mechanics Rotational Inertia n An object rotating about an axis tends to remain rotating unless interfered with by some external.
Chapter 10: Rotation. Rotational Variables Radian Measure Angular Displacement Angular Velocity Angular Acceleration.
Phy 211: General Physics I Chapter 10: Rotation Lecture Notes.
Physics Announcements WebAssign – –Chapter 7 due today Exam #2 not graded yet Picture: 30-m Darrieus Wind turbine in the Magdalen Islands.
Kinematics, Momentum and Energy BU Photon Outreach December 14, 2010.
Phy 201: General Physics I Chapter 9: Rotational Dynamics Lecture Notes.
ROTATIONAL MOTION.
\Rotational Motion. Rotational Inertia and Newton’s Second Law  In linear motion, net force and mass determine the acceleration of an object.  For rotational.
Rotation of rigid objects- object with definite shape
 Torque: the ability of a force to cause a body to rotate about a particular axis.  Torque is also written as: Fl = Flsin = F l  Torque= force x.
Physics 1210/1310 Mechanics& Thermodynamics Thermodynamics Lecture R1-7 Rotational Motion.
8.4. Newton’s Second Law for Rotational Motion
Chapter 9: Rotational Dynamics
Torque Chap 8 Units: m N 2.
Rotational Motion. Deg, Rad, Grad There are 360 degrees in one rotation of a circe. There are 2π radians in one rotation of a circle. There are 400 gradians.
Notes on Chapter Center of Gravity & Rotational Mechanics
Chapter 8 Rotational Motion.
Biomechanics Part 2.
Rotational Motion. Tangential and Rotational Velocity.
Chapter 8 Rotational Motion.
Rotational Mechanics. Rotary Motion Rotation about internal axis (spinning) Rate of rotation can be constant or variable Use angular variables to describe.
ROTATIONAL MECHANICS And the fun continues…. A torque is produced when a force is applied with “leverage.” – Ex. You use leverage when you pull a nail.
Types of Motion Topic 4 – Movement Analysis
Chapter 11 Rotational Mechanics. Recall: If you want an object to move, you apply a FORCE.
Rotational Kinetic Energy An object rotating about some axis with an angular speed, , has rotational kinetic energy even though it may not have.
Seesaws.
8.2 Rotational Dynamics How do you get a ruler to spin on the end of a pencil? Apply a force perpendicular to the ruler. The ruler is the lever arm How.
Circular Motion. Rotation and Revolution When a body turns about it’s axis is known as a rotation. When a body turns about it’s axis is known as a rotation.
MOMENTUM l Momentum is a measure of motion =“magnitude of motion”, “impetus”, “impulse” p = m  v rate of change of momentum = force: if no force acts,
Angular Mechanics Chapter 8/9 Similarities LinearAngular MassMoment of Inertia ForceTorque MomentumAngular Momentum.
Chapter 9 Rotational Dynamics.
Circular Motion, Center of Gravity, & Rotational Mechanics
Chapter 9 Rotational Dynamics
Physics Formulas. The Components of a Vector Can resolve vector into perpendicular components using a two-dimensional coordinate system:
Rotational Dynamics Rode, Kiana, Tiana, and Celina.
Rotating objects tend to keep rotating while non-rotating objects tend to remain non- rotating.
Rotational Inertia Chapter Notes. Rotational Inertia Newton’s 1 st law (law of inertia) states that an object in motion remains in motion, and.
Angular Momentum Chapter Notes. Angular Momentum Recall that linear momentum is equal to an object’s mass times its velocity Anything that rotates.
Elizabeth, Colby, Ashley, Brittany. State and Explain Concepts  Torque is the tendency of a force to cause rotation about an axis.  Lever arm is he.
Application of Forces Learning Objectives:
Ch 8 : Rotational Motion .
CONCEPTUAL PHYSICS Rotational Mechanics.
Rotational Motion Rotational Inertia – inertia is how an object resists changing its motion so rotational inertia is how much an object resists changing.
College Physics, 7th Edition
Angular Momentum.
Rotational Inertia and Torque
Rotational Dynamics Chapter 9.
"I think that was the game we discovered Gary Russell as a potential short-yardage and goal-line runner," Tomlin said. "And that's been solid for us. We.
Chapter 8 Rotational Motion
Chapter 11 Rotational Mechanics.
Makenna Cooper, Lukas Binau, Savannah Sharp, Alexis Lundy
Chapter 8 Rotational Motion.
Chapter 11 - Rotational Dynamics
Think of it as rotational _________________.
Presentation transcript:

Cheyanne Rimer, Jeremy Massari, William Ortiz, Jordan Cooper, and Duncan Godsey Rotational Mechanics

Torque Torque is produced when a force is applied with leverage. Leverage is the exertion of force by means of a lever or an object used in the manner of a lever. When the force that is being applied is perpendicular, the distance from the turning axis to the point of contact is the lever arm.

Torque Continued Torque is not the same as force. The angle of the force being applied is important. If the force is not at a right angle to the lever arm, then only the perpendicular component of force will contribute to the torque. torque=force(perpendicular angle)X lever arm.

Torque and Center of Gravity When attempting to touch your toes while leaning against a wall, you will find yourself falling over. You fall because there is no base support underneath the center of gravity and because of torque. When the area bounded by your feet is not beneath of center of gravity, that is an example of torque.

Rotational Inertia The resistance of an object to changes in its rotational state of motion is rotational inertia. Rotating objects tend to keep rotating, while nonrotating objects tend to stay nonrotating. Formula: I=mr^2 M=mass, r=distance from a rotational axis. Depending on the object, the formula will change.

Will a hollow or solid cylinder roll faster? The object with the smaller rotational inertia will roll faster. The object with greater rotational inertia will require more time to get rolling. But which has more rotational inertia? The solid or hollow cylinder? The hollow cylinder has a greater rotational inertia therefore the solid cylinder will roll with greater acceleration.

Angular Momentum The product of the momentum of inertia of a body about an axis and its angular velocity at the same axis. When a direction is assigned to rotational speed it is called rotational velocity. The “inertia of rotation” of rotating objects is also called angular momentum.

Angular Momentum Continued Angular momentum=mvr mv is the angular momentum is equal to the magnitude of its linear momentum, while r is the radial distance. Linear momentum= mass X velocity

Conservation of Angular momentum This law states that if no unbalanced external torque acts on a rotating system, the angular momentum of the system is constant. In other words the product of rotational inertia and rotational velocity at one time will be the same as at any other time.