(composed by Steve Reich) - University Of Maryland … · 4/8/11 Physics 122 17 Field of force felt...

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4/8/11 1 Physics 122 (composed by Steve Reich)

Transcript of (composed by Steve Reich) - University Of Maryland … · 4/8/11 Physics 122 17 Field of force felt...

4/8/11 1 Physics 122

(composed by Steve Reich)

4/14/10 11 Physics 122

Δ12 mv2( ) = F||

netΔr = Fnet iΔr = W net

ii WU =Δ−

4/8/11 13 Physics 122

ΔUE = −FE ⋅ Δr (small step)

ΔUE = − FE ⋅ Δr( )∑ (lots of little steps)

ΔUE = − FE ⋅drstart

finish

General case

Simplest case (one source charge, one test charge)

ΔUE = − FE ⋅drstart

finish

∫ = −kCqQ

r2dr

ri

rf

∫ = −kCqQdr

r2ri

rf

∫ = −kCqQ1

ri

−1

rf

⎝⎜⎞

⎠⎟

UE (r) =kCqQ

rNOT A VECTOR – JUST A NUMBER

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Field of force felt by a positive test charge near a positive source.

Electric Field felt by a positive test charge near a positive source.

F =kqQ

r2

E =kQ

r2

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Field of force felt by a negative test charge near a positive source.

Electric Field felt by a negative test charge near a positive source.

F =kqQ

r2

E =kQ

r2

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qUV

qFE ==

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Potential energy of a positive test charge near a positive source.

Electric Potential of a positive test charge near a positive source.

U =kqQ

r

V =kQ

r

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Potential energy of a positive test charge near a positive source.

Electric Potential of a positive test charge near a positive source.

U =kqQ

r

V =kQ

r

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Δ( 12 mv2 ) = Fnet ⋅ Δr

= mg ⋅ Δr

= −mg Δh

ΔUgrav = mgΔh

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ΔU = −FiΔr

F = −ΔU

Δr(stepping in the direction

of the steepest descent)

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g =

F

mVgrav =

Ugrav

m= gh

Not equal!

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r

rto∞