Electrostatic Potential and Capacitance

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New answer posted•a year ago
S
a year ago

F R = { k Q q 0 ( a − x ) 2 − k Q q 0 ( a + x ) 2 }

= − k Q q 0 { a 2 + x 2 + 2 a x − a 2 − x 2 + 2 a x ( a 2 − x 2 ) }

F R = − k Q q 0 ( 4 a x ) ( a 2 − x 2 ) 2

T = 2 π a 3 m 4 k Q q 0 = 4 π 2 a 3 m × 4 π ε 0 4 Q q 0 = 4 π 3 ε 0 m a 3 Q q 0 .                          

   

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New answer posted•a year ago
New answer posted•a year ago
S
a year ago

For sphere ‘C’ after contacting with ‘A’. qA = qC = q2.

offer contacting with ‘B’. qB = qC = 3q4

FNet=|F1−F2|

F2 = K⋅3q2×4r28=32kq2r2

F1=9kq2×416r2=9kq24r2=94F

∴FNet=|94F−32F|

= 9−64F=34F

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New answer posted•a year ago
S
a year ago

Q = CV

= 50 × 10-12 × 100

= 5 × 10-12 × 103

Q = 5 × 10-9C

Ui           (Initial Energy)  

=  Q 2 2 C = 2 5 × 1 0 − 1 8 2 × 5 0 × 1 0 − 1 2

=  1 4 × 1 0 − 6

Now capacitor is connected to an identical uncharged capacitor

kvL

Q 1 C = Q 2 C = 0    

q1 = q2

Initial change Q1 + Q2 = Q

⇒ 2 Q 1 = Q     &nb

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New answer posted•a year ago
S
a year ago

F = q E [ E = σ ε 0 ]

F = q σ ∈ 0 = 1 0 N

Final case – Now one plate is removed, Electric field will becomes half; So, force will become half.

F ' = 1 0 2 = 5 N

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New answer posted•a year ago
S
a year ago

In forward bias diode act as a short circuit wire. Hence, the equivalent circuit is now.

So,   V a b = 30 5 + 10 * 5 = 10 V

50.00

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New answer posted•a year ago
New answer posted•a year ago
S
a year ago

Electric Displacement

D → = ∈ o E → [ D ] = [ ∈ 0 E → ] = [ ∈ 0 σ ∈ 0 ] [ D ] = [ σ ]

Electric displacement ( D → )  and surface change density

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New answer posted•a year ago
New answer posted•a year ago
S
a year ago

K  V  L Loop 1               

   

6 - l × 1   -l1 × 1 - 4 = 0

2 = l + l1                     

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