Full Contact Learning
Employing the body as a learning tool
Mary Bridget Kustusch and Susan Fischer
DePaul University Teaching and Learning Conference 2 May 2014
Full Contact Learning Employing the body as a learning tool Mary - - PowerPoint PPT Presentation
Full Contact Learning Employing the body as a learning tool Mary Bridget Kustusch and Susan Fischer DePaul University Teaching and Learning Conference 2 May 2014 Embodied Cognition In an embodied cognition perspective, all abstractions
DePaul University Teaching and Learning Conference 2 May 2014
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For rotational motion: linear momentum = (mass)*(velocity) p = mv angular momentum = (moment of inertia)*(angular velocity) L = Iω What is the moment of inertia
Rulers + Binder clips!
espn.go.com/nhl/tesm/photos
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It is harder to “flip” the ruler the further the binder clip is from the pivot point. “Harder” means a larger moment of inertia. If you change the location of the pivot point, you affect the difficulty in “flipping” the ruler. The moment of inertia of an object depends
The moment of inertia of an object depends on where the pivot point (or axis of rotation) is.
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The two identical solid cylinders shown below are spinning about different axes. Which configuration has the larger Moment of Inertia?
A B
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How does this apply to angular momentum and ice skaters? Compare what is happening when the skater first starts spinning, and when the skater is about to finish the spin. What changes? What can we learn about angular momentum? (angular momentum) = (moment of inertia) * (angular velocity)
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Feeling 1-dimensional motion Using a bicycle wheel to feel changes in angular momentum
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“building” DNA Energy Theater
ete particles.
Creating non-linear charge density
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The life cycle of a star Flow of charges in a uniform current density Energy transfers & transformations for a hand pushing a box across a floor at constant speed. Sky Time: relationship between time and astronomical motion
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Transverse Waves Time evolution of a complex 2-state system Acting out the meter of a poem
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