A thin disk of radius a carries a uniform surface charge density p [C/m²]. Find the energy required to move a negative point charge -q from a point very far from the disk (infinity) to a final position along its axis, a distance h from the center of the disk as shown. This can be done two ways using knowledge of the field and Y Z h--q a Pso

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A thin disk of radius a carries a uniform surface charge
density po [C/m²]. Find the energy required to move a
negative point charge -q from a point very far from the
disk (infinity) to a final position along its axis, a
distance h from the center of the disk as shown. This
can be done two ways using knowledge of the field and
potential of a uniformly-charged disk, which is derived
in the lecture slides. What is the force on the charge in
its final resting position? What is the net force on
the disk?
X
h--q
a
-Pso
y
Transcribed Image Text:A thin disk of radius a carries a uniform surface charge density po [C/m²]. Find the energy required to move a negative point charge -q from a point very far from the disk (infinity) to a final position along its axis, a distance h from the center of the disk as shown. This can be done two ways using knowledge of the field and potential of a uniformly-charged disk, which is derived in the lecture slides. What is the force on the charge in its final resting position? What is the net force on the disk? X h--q a -Pso y
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Solution:

Let P be the point at a distance h from the disc. The potential at point P due to a uniformly charged thin disc is given by,

Vp=ρ2ε0h2+a2-h

The energy required to move a negative charge -q to the point P from infinity is given by,

E=Uf-Ui   =-qVp-0   =-qρ2ε0h2+a2-h

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