
Chapter 4
... to its mass multiplied by the rate of change of its velocity. D. The force on a mass is equal to the distance pushed times work done on the mass. ...
... to its mass multiplied by the rate of change of its velocity. D. The force on a mass is equal to the distance pushed times work done on the mass. ...
STP 111 THEOR - Unesco
... 1.10 Write and explain the expression for the kinetic energy of rotation of a rigid body A rotating rigid body consist of mass in motion, so it has K.E. We can express this K.E in term of the body’s angular speed and a new quantity, called Moment of Inertia, that depends on the body’s mass and how t ...
... 1.10 Write and explain the expression for the kinetic energy of rotation of a rigid body A rotating rigid body consist of mass in motion, so it has K.E. We can express this K.E in term of the body’s angular speed and a new quantity, called Moment of Inertia, that depends on the body’s mass and how t ...
Forces and Motion
... The larger the object is, the more we are effected by its gravitational pull. We are more attracted to the Earth’s gravity than we are to gravity of the things in the room ...
... The larger the object is, the more we are effected by its gravitational pull. We are more attracted to the Earth’s gravity than we are to gravity of the things in the room ...
Forces! - Ottawa Hills Local School District
... • An example of a balance force is when you have a arm wrestle with someone that is strong as you are and you guys are pushing as hard as you can and your arms stay in the same place. • Unbalanced force is always cause a change in motion • Unbalanced forces can cause the opposing forces to slow down ...
... • An example of a balance force is when you have a arm wrestle with someone that is strong as you are and you guys are pushing as hard as you can and your arms stay in the same place. • Unbalanced force is always cause a change in motion • Unbalanced forces can cause the opposing forces to slow down ...
Jeopardy
... speed was constant and it moved in the same direction so its velocity did not change either. ...
... speed was constant and it moved in the same direction so its velocity did not change either. ...
ForcedVibrations-freestudy-co-uk.pdf
... The spring force is directly proportional to displacement x so it must be in phase with x. The damping force is directly proportional to the velocity v so it must be in phase with v. The inertia force is directly proportional to the acceleration a so it must be in phase with a. It follows that the t ...
... The spring force is directly proportional to displacement x so it must be in phase with x. The damping force is directly proportional to the velocity v so it must be in phase with v. The inertia force is directly proportional to the acceleration a so it must be in phase with a. It follows that the t ...
Day 4
... The force of the car on the truck is equal and ! opposite to the force of the truck on the car. T •! The momentum transferred from the truck to ! the car is equal and opposite to the momentum ! transferred from the car to the truck. T •! The change of velocity of the car is the same as ! the change ...
... The force of the car on the truck is equal and ! opposite to the force of the truck on the car. T •! The momentum transferred from the truck to ! the car is equal and opposite to the momentum ! transferred from the car to the truck. T •! The change of velocity of the car is the same as ! the change ...
Mechanical Vibrations
... • When the motion is maintained by the restoring forces only, the vibration is described as free vibration. When a periodic force is applied to the system, the motion is described as forced vibration. • When the frictional dissipation of energy is neglected, the motion is said to be undamped. Actual ...
... • When the motion is maintained by the restoring forces only, the vibration is described as free vibration. When a periodic force is applied to the system, the motion is described as forced vibration. • When the frictional dissipation of energy is neglected, the motion is said to be undamped. Actual ...
Classical central-force problem
In classical mechanics, the central-force problem is to determine the motion of a particle under the influence of a single central force. A central force is a force that points from the particle directly towards (or directly away from) a fixed point in space, the center, and whose magnitude only depends on the distance of the object to the center. In many important cases, the problem can be solved analytically, i.e., in terms of well-studied functions such as trigonometric functions.The solution of this problem is important to classical physics, since many naturally occurring forces are central. Examples include gravity and electromagnetism as described by Newton's law of universal gravitation and Coulomb's law, respectively. The problem is also important because some more complicated problems in classical physics (such as the two-body problem with forces along the line connecting the two bodies) can be reduced to a central-force problem. Finally, the solution to the central-force problem often makes a good initial approximation of the true motion, as in calculating the motion of the planets in the Solar System.