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02 Electric Fields and MotionofCharges-2021-2

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Thanuxsan Anton
Chilcodi CharlesObi
Rogan Scanlan
ti
2
6
Et
E3
k
T
T
Es
N
From Qato
From
Me 3mi
Qatop
1 2mg
FromQatop
13 21 1 sj
Labeledin Blue
I
f
P
is
j
13 73
21 1 si
V2 so
0.87 0.6
This information was notneeded because themagnitude and signare
notnecessary they are only needed to calculate the electricfold
The electric Krld du Qa is to the
right i
downward
the electricfold du Qa is
and theelectricfold dm Q is in the direction of
j
f
Labeledin
green
T
j
1
12.304
4s
2.220
I 3041 6.2285
Ng
Notherecouldnot beanequilibriumpoint as themagnitude of the
chargecombined w theirseparation doesnotcomeout to an equilibrium point
Basedon
the prediction theactualchargewouldhe 0.4 orlessaccording
tothesimulation
3 AV 930 P
3.9 1.6 1019 6.24x W a
870fromthepositive x
axis
Theequilibrium wouldnot bestable because the charge at thepoint
is positin making the foldnetorpoint
awayfrom thecharge
The equilibrium would be stable because thechargeat thepoint
is negative making the feildwetor point in the direction ofthecharge
It wouldnotbepossible tocreate apoint that is stable for displacements in
3D using static electric charges in 2b duetothefactthat thefoldsaremeant to
thecharges
surround
while thefoldmotorsdobecome parallel tothetrajectorynearthestartandtheend
nearthenegativepoint charge all of the E Bildwatorspointdirectly to it
Anargumentthatcanbemade astowhythe puckdoesnot
outsideforcesactingonthe charge inthesimulation
Th
arrangenut wouldnot giveus agoalunlessall
madeopposite aswell
follow th
E foldlines duto
ofthechargeswere
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