'Point o' presentation slideshows

Chapter 27: Sources of the Magnetic Field

Chapter 27: Sources of the Magnetic Field . Section 27-1: The Magnetic Field of Moving Point Charges.

1.52k views • 88 slides

1.41k views • 65 slides

Oscillation

Oscillation. Oscillations of a Spring S imple H armonic M otion Energy in the Simple Harmonic Oscillator Simple Harmonic Motion Related to Uniform Circular Motion The Simple Pendulum The Physical Pendulum and the Torsion Pendulum Damped Harmonic Motion Forced Oscillations; Resonance.

995 views • 64 slides

Drying

3.55k views • 53 slides

MOMENT OF A FORCE (Section 4.1)

1.27k views • 43 slides

All figures taken from Vector Mechanics for Engineers: Dynamics , Beer and Johnston, 2004

ENGR 214 Chapter 17 Plane Motion of Rigid Bodies: Energy & Momentum Methods. All figures taken from Vector Mechanics for Engineers: Dynamics , Beer and Johnston, 2004. Principle of Work and Energy for a Rigid Body. initial and final total kinetic energy of rigid body.

900 views • 42 slides

Kinetics of Particles Impulse and Momentum

Kinetics of Particles Impulse and Momentum. Linear Impulse and Linear Momentum. Consider the general curvilinear motion in space of a particle of mass m , where the particle is located by its position vector measured from a fixed origin O.

1.56k views • 29 slides

CHAPTER 15

CHAPTER 15. Kinematics of Rigid Bodies. translation:. rectilinear translation. curvilinear translation. rotation about a fixed axis. general plane motion. motion about a fixed point. Introduction.

1.5k views • 28 slides

This was the homework from last time: Complete reading Chapter 2

This was the homework from last time: Complete reading Chapter 2 Exercise: 15a and revisit exercise 10. Major Exercises: 4 a, b, 7 Begin thinking about the Problem Set (which you will have time to complete in class next time). Definition

487 views • 27 slides

Systems of Particles

687 views • 26 slides

Lecture #8

Lecture #8. Distributed Loads Reference Chapter 4, Section 9. 1. The resultant force (F R ) due to a distributed load is equivalent to the _____ under the distributed loading curve, w = w(x). A) Centroid B) Arc length C) Area D) Volume. Distributed load curve. w. x. F. R.

306 views • 20 slides

Torque

557 views • 20 slides

Moment of a force

3.19k views • 18 slides

EQUATIONS OF EQUILIBRIUM & TWO- AND THREE-FORCE MEMEBERS

519 views • 17 slides

Lecture 14 Mirrors

Lecture 14 Mirrors. Chapter 23.1 ? 23.3. Outline. Flat Mirrors Spherical Concave Mirrors Spherical Convex Mirrors. Flat Mirrors. p. q. Source of light is placed at point O at a distance p from a flat mirror. Point I is the image of point O . q is the image distance.

374 views • 13 slides

Physics 430: Lecture 20 Non-Inertial Frames

Physics 430: Lecture 20 Non-Inertial Frames. Dale E. Gary NJIT Physics Department. 9.1 Acceleration without Rotation. It is sometimes useful to work in non-inertial frames, but in order to do that we have to make some changes to the equations we developed for inertial frames up to now.

697 views • 12 slides

Velocity - time graph

1.59k views • 8 slides

305 views • 5 slides

BEARINGS

246 views • 3 slides

BEARINGS

460 views • 3 slides