1 / 7

Announcements

Announcements. HW#4 on Ch. 5 due tonight Remember the 1 st midterm, Weds., Feb. 25 , Covers chapters 1-5 No makeup tests. F. F r. F t. Forces in Non-uniform Circular Motion. The object has both tangential and radial accelerations. What does this statement mean?.

twilmoth
Télécharger la présentation

Announcements

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Announcements • HW#4 on Ch. 5 due tonight • Remember the 1st midterm, Weds., Feb. 25, • Covers chapters 1-5 • No makeup tests PHYS 1443-501, Spring 2004 Dr. Andrew Brandt

  2. F Fr Ft Forces in Non-uniform Circular Motion The object has both tangential and radial accelerations. What does this statement mean? The object is moving under both tangential and radial forces. These forces cause not only the velocity but also the speed of the ball to change. The object undergoes a curved motion under the absence of constraints, such as a string. How does the acceleration look? PHYS 1443-501, Spring 2004 Dr. Andrew Brandt

  3. Motion with Resistive Forces A medium can exert resistive forces on an object moving through it due to viscosity or other types frictional properties of the medium. Some examples? Air resistance, viscous force of liquid, etc These forces are exerted on moving objects in the opposite direction of the motion. These forces are proportional to such factors as speed. They almost always increase with increasing speed. • Two different cases of proportionality: • Forces linearly proportional to speed: Slowly moving or very small objects • Forces proportional to square of speed: Large objects w/ reasonable speed PHYS 1443-501, Spring 2004 Dr. Andrew Brandt

  4. R v mg Resistive Force Proportional to Speed Since the resistive force is proportional to speed, we can write R=bv Let’s consider that a ball of mass m is falling through a liquid. m This equation also tells you that What does this mean? The above equation also tells us that as time goes on the speed increases and the acceleration decreases, eventually reaching 0. An object moving in a viscous medium will obtain speed to a certain speed (terminal speed) and then maintain the same speed without any more acceleration. What is the terminal speed in above case? The time needed to reach 63.2% of the terminal speed is defined as the time constant, t=m/b. How do the speed and acceleration depend on time? PHYS 1443-501, Spring 2004 Dr. Andrew Brandt

  5. Review: Lectures 1-3 Significant figures, displacement, velocity, acceleration, 1-D motion, free fall, constant acceleration equations: Velocity as a function of time Displacement as a function of velocity and time Displacement as a function of time, velocity, and acceleration Velocity as a function of displacement and acceleration PHYS 1443-501, Spring 2004 Dr. Andrew Brandt

  6. Lectures 4-6 Coordinate systems, vectors (defn., operations, components unit vectors), 2-D motion, projectile motion, reference frames Range+Max height PHYS 1443-501, Spring 2004 Dr. Andrew Brandt

  7. Lectures 6-9 Force, Newton’s Laws, weight, free body diagrams, inclined planes, pulleys, friction, circular motion. PHYS 1443-501, Spring 2004 Dr. Andrew Brandt

More Related