(composed by Steve Reich) - University Of Maryland … · 4/8/11 Physics 122 17 Field of force felt...
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Transcript of (composed by Steve Reich) - University Of Maryland … · 4/8/11 Physics 122 17 Field of force felt...
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
4/8/11 15 Physics 122
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
4/8/11 17 Physics 122
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
4/8/11 19 Physics 122
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
4/8/11 20 Physics 122
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