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Physics Human Density Lab 2012

Honza and his microwave show

 

Amazing Theatre of Physics

Performed at The Nicholas Copernicus Observatory and Planetarium in Brno, November 2008

Critical thinking labs in intro physics

Natasha Holmes – Stanford University

NCNAAPT Spring 2016 Conference at Foothill College

Critical thinking labs in intro physics

Natasha Holmes – Stanford University

NCNAAPT Spring 2016 Section Meeting & Conference at Foothill College

Physics Human Density Lab 2012

COLLAPSE OF MATTER COMPARISONS BY RICHARD LAZZARA

Original Sumi-e Pen & Ink Calligraphy Cards by Richard Lazzara

www.flickr.com/photos/shankargallery/sets/72157594518634150/

NCNAAPT Spring 2016 Conference at Foothill College

Start study physics from day one to improve yourself in physics in your school and competitive exam

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NEET/IIT/IB

KUMAR PHYSICS CLASSES

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CBSE/IIT/SAT PHYSICS/AP’S PHYSICS CLASSES

WITH CONCEPT BUILDING

Bree Barnett Dreyfuss shares an electrophorus build activity.

Department of Physics, Bangladesh University of Engineering and Technology (BUET). I didn't even know Buet had a Dept. of Physics. My cousin was working with her thesis at the department. The building is one of the oldest in the university.

Physics Photography Project

Spring Conference and meeting at Contra Costa College

APS Conference for Undergraduate Women in Physics at Georgia Tech

 

cuwip.physics.gatech.edu/

 

Copyright Predrag Cvitanović

Jenni Guzman, our keynote speaker, speaking on gender bias in Physics

How hard or soft should I throw this in order to get the pins?

Physics Human Density Lab 2012

Rube Goldberg Competition 2016

We set the scanner under a slow moving ceiling fan. You can see the blades equally spaced the whole way.

Growing in the top of the cold trap dewar.

Physics labs are so useful for all majors...

This is where I live now. I've posted this same picture on the Davis wiki site (daviswiki.org) on my user page, except with green overlaid on the dirt so I feel like it's prettier than it is...

DoseNet: Building scientific literacy through a network of radiation detection devices

Ali Hanks – UC Berkeley

NCNAAPT Spring 2016 Conference at Foothill College

APS Conference for Undergraduate Women in Physics at Georgia Tech

 

cuwip.physics.gatech.edu/

 

Copyright Predrag Cvitanović

Physics Human Density Lab 2012

Valerie Risk shares her homemade momentum carts

Ann Hicks of PASCO explains the raffle prizes they donated.

Rotational Motion Physics Classes/Tutor In Kalkaji/Gk 2/C r Park/GK 1-Kumar Sir-9958461445

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Rotational Motion Physics Class 11 Chart

  

A rigid body is an object of finite extent in which all the distances between the component particles are constant. No truly rigid body exists; external forces can deform any solid. For our purposes, then, a rigid body is a solid which requires large forces to deform it appreciably.

  

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A change in the position of a particle in three-dimensional space can be completely specified by three coordinates. A change in the position of a rigid body is more complicated to describe. It can be regarded as a combination of two distinct types of motion: translational motion and rotational motion.

  

Purely translational motion occurs when every particle of the body has the same instantaneous velocity as every other particle; then the path traced out by any particle is exactly parallel to the path traced out by every other particle in the body. Under translational motion, the change in the position of a rigid body is specified completely by three coordinates such as x, y, and z giving the displacement of any point, such as the center of mass, fixed to the rigid body.

  

Purely rotational motion occurs if every particle in the body moves in a circle about a single line. This line is called the axis of rotation. Then the radius vectors from the axis to all particles undergo the same angular displacement in the same time. The axis of rotation need not go through the body. In general, any rotation can be specified completely by the three angular displacements with respect to the rectangular-coordinate axes x, y, and z. Any change in the position of the rigid body is thus completely described by three translational and three rotational coordinates.

  

Any displacement of a rigid body may be arrived at by first subjecting the body to a displacement followed by a rotation, or conversely, to a rotation followed by a displacement. We already know that for any collection of particles—whether at rest with respect to one another, as in a rigid body, or in relative motion, like the exploding fragments of a shell, the acceleration of the center of mass is given by

  

Fnet=MacmF_{{{\mathrm {net}}}}=Ma_{{{\mathrm {cm}}}}\;\!

where M is the total mass of the system and acm is the acceleration of the centre of mass. There remains the matter of describing the rotation of the body about the centre of mass and relating it to the external forces acting on the body. The kinematics and dynamics of rotational motion around a single axis resemble the kinematics and dynamics of translational motion; rotational motion around a single axis even has a work-energy theorem analogous to that of particle dynamics.

  

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