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♣#$♦
② ♦♦♠
!♦♠
♦" ♦&" )♥&" &♥♥ ♥ ♠" m ② 0 q ♥♦ " ♣♦♥♥ ♥ ♥ &③6♥ ")0♦ 0♦ R ♦♥ ♣0" ♥♦ ♦♥&♦0" ② "♥ 06♥ " ♦&" " ♠♥ "& ; ♥
♣♦"6♥ ;0♦ "&<♥ "♣0" ♣♦0 ♥ "&♥ R &0♠♥ " 0" " ♦&"
♦-♥
=0 ♣0 ♦♥6♥ ;0♦ " ♥"0♦ ; "0♠♦" &♦" " 0③" "♦0 ♥
" ♦&" 0" =0 "&♦ ♦♥"0♠♦" "♥& ♦♥06♥ ♣0 ♣0♦♠
0③ ♥♦0♠
~N " ♣ "00 "♥♦ "" ♦♠♣♦♥♥&" 0&♥0" ♦♠♦
~N = N cos(π/3)i + N sin(π/3)j
0③
~Fe " 0 ♣♦0 ♦& 0 "♦0 ♦& ③;0 ② "
~Fe =kq2
R2
"❮❯ ❨ ❯
♦$ &♠♠♦& $③& ♣♦$ ♦♠♣♦♥♥/ &♦$ ♦/ $ ② ♣♠♦& ♦♥5♥
6$♦
$③ ♥ ❳
∑
FX = N cos(π/3)− kq2
R2= 0 (1)
$③ ♥ ❨
∑
FY = N sin(π/3)−mg = 0 (2)
♠♦& 6
N =mg
sin(π/3)
♠♣③♥♦ &/ ①♣$&♦♥ ♥
mg
sin(π/3)cos(π/3)− kq2
R2= 0
&♣♥♦ q
q = ±R
√
mg cot(π/3)
k
!♦♠
#♥♥ ♦( ♠(( ( ♠ ♠(♠ / 0 ♥( #/2( ♥ (♠♥#♦ /# ♦
♠( ♥/♦/ (#8 ①#/♠♦ ♥/♦/ (♠♥#♦ ② ♠( (♣/♦/ ( ♣ ♠♦/
/♠♥#
♥♥#/ ♣♦(?♥ 0/♦ ♠( (♣/♦/
♥♥#/ /♥ ♣0@( ♦(♦♥( ♠( ♥ #♦/♥♦ ( ♣♥#♦
0/♦
♦-♥
( /( 2#/( (♦♥ ♠(♠♦ (♥♦ ♣♦/ ♦ 0 /③ 2#/ ♥#/ ♠( (
/♣( (D ♠( (♣/♦/ ①♣/♠♥# ♥ /③ 2#/ // ② ( ♣(♦
♦ (#♥♦ ♥ 0/♦ ♥♦ ♠( /③( (♦♥ ( ♦♥(/♥♦ (#♦
#♥♠♦(
mg = kq2
x02
♦♥ x0 ♣♦(?♥ 0/♦
=⇒ x0 = q ·√
k
mg(1)
♦♥(/♠♦( ♥ ♦♦/♥ ① ♥ #♦/♥♦ ♣♦(?♥ 0/♦ x0 ♥♠♦( ♣♦/
② #?♥
F = md2x
dt2= −mg +
kq2
(x0 + x)2
K/ ♦(♦♥( ♣0@( |x| << |x0| =⇒ | xx0| << 1 ♣♦/ ♦ 0
F = md2x
dt2= −mg +
kq2
(x0 + x)2= −mg +
kq2
x02· (1 +
x
x0)−2 ∼= −mg +
kq2
x02· (1− 2
x
x0)
K/♦ #♥♠♦( 0 mg = kq2
x02
=⇒ md2x
dt2∼= −2kq2x
x03
=⇒ d2x
dt2+
2kq2
mx02· x
x0= 0
K/♦ mx02 = kq2
g
=⇒ d2x
dt2+
2g
x0· x = 0
K♦/ #♥#♦ #♥♠♦( 0 /♥ ♦(♦♥( ♣0@( (
w =
√
2g
x0
"❮❯ ❨ ❯
!♦♠
♥ ♦% '()% ♥ )(/♥♦ 1/)(♦ ♦ ② )(% (% ♥)% 1 % ♣♦♥
♥ ( ♥ ♥)(♦ ( )(/♥♦ ♥♥)( ) 1 %%)♠ %)' ♥
1(♦ ( (
♦-♥ (♠♦% ♥♦♥)(( ) 1 (③ ♥ ♦% '()% % (♦ ♦♠♠♦% x
(D♥ ( ③1( ♥(♦( ( ♥(♦( ② y ♣♥)♦ ♠♦ ♦
♥(♦( ( '() %♣(♦( %)D♥ % ♥/♦ ♥ ♦% )(% '()% ♥)('♠♦♥♦%
♥ ( ( ♥(♦( ♥♠♦% 1 % (③% ')(% 1 ①♣(♠♥) %♦♥
~F1 = kq2
L2· (cos(π
3)x− sen(
π
3)y) = k
q2
L2· ( x
2−√
3
2y)
~F2 = kq2
L2x
(③ (%)♥) %
~F = ~F1 + ~F2 =3
2k
q2
L2x−
√3
2k
q2
L2y =
√3 · k q2
L2· (√
3
2x− y
2) =
√3 · k q2
L2· (cos(π
6)x− sen(
π
6)y)
%♥)♦ (③ ♠♦% 1 %( ♣♦%) ♦( ♦♠)(I ♠♥) %)♦
% )♦( ♣♦♠♦% ( 1 (③ ♥)( ② 1 )♥ (D♥ π − π6 (%♣)♦ x
♣♦( ♦ 1 (③ %♦( 1 ♦ % ♦)(% (% ♥)% % ♥)♣( ♦♥ (③
')( %♦( 1 ♦ % ♥)(D♥ ♦♥ %I ♣( 1 1 %)' ♥ 1(♦ ♥♦% %)
( ♦% ♠D♦% % (③%
%)♥ ♥)( 1 ② ♣♦♠♦% ♥♦♥)(( %♥♦ ② ♦% %♥♦% %♦( )(/♥♦
1 1 % % )(/♥♦ 1/)(♦ %I
r
sen(π6 )
=L
sen(2π3 )
=⇒ r =L√3
K♦( )♥)♦ ( ♦% ♠D♦% % (③% ♦)♥♠♦%
√3 · k q2
L2= k
( L√
3)2
=⇒ Q =1√3· q
!♦♠
♦# &# ♣♥+# ♣♦#+# #+1♥ #♣&# ♣♦& ♥ #+♥ 2a 4♦& ♣♥+♦ ♠♦
#♠♥+♦ 6 # ♥ # +&③ ♥ ♣♥♦ ♣&♣♥& ♠#♠♦ & ♦# ♣♥+♦# ♥ 6
&③ #♦& ♥ & ♣& 6 ♥ ♣♥♦ # ♠1①♠ # ♣♦& #♠+&< ♥ &♥&♥
♥♥+& &♦ &♥&♥
♦-♥
#♠+&< ♣&♦♠ ♥+♠♥♦ #♠♦# 6 &③ #♦& & ♣& #+1
#♦& ♣♥♦ + ♣♥♦ ♣♥♦ ①② ♦♦&♥# &+#♥# ② ♣♦♥♠♦# ♠# &#
#♦& ③ #+ ♦&♠ +♥♠♦# 6 ~r = R · (cos(θ)x + sen(θ)y) ~r1 = az ② ~r2 = −az♦♥ ~r # ♣♦#B♥ & ♣& ② ~r1, ~r2 #♦♥ # ♣♦#♦♥# # &# ♣♦#+#
♥+# ♠♥♦♥# ♠1# |~r− ~r1| = |~r− ~r2| =√
R2 + a2 &③ E+& #♦& &
♣& #
~F = ~F1 + ~F2 =kqQ
(R2 + a2)3
2
· (Rcos(θ)x + Rsen(θ)y − az + Rcos(θ)x + Rsen(θ)y + az)
=2kqQR
(R2 + a2)3
2
· (cos(θ)x + sen(θ)y) .
#+♦ ♠♦# 6 &③ #♦& & ♣& #+1 #♦& ♣♥♦ &♠♥+ ♦ 6
♠♦# & # ♠①♠③& ♠B♦ #+ &③ ② ♥♦♥+&& ♦♥ ♦ & ♦♠E+&♦
#&+♦ ♣♦& ♦# ♣♥+♦# ♦♥ ♠B♦ #+ &③ # ♠1①♠ # & ♠♦# ♠①♠③&
♥B♥
|~F | = 2kqQR
(R2 + a2)3
2
= 2kqQ · f(R)
=⇒ df(R)
dR=
(R2 + a2)3
2 − 3R2(R2 + a2)1
2
(R2 + a2)3= 0
=⇒ (R2 + a2)1
2 · ((R2 + a2)− 3R2)) = 0 =⇒ R =1√2· a
❱♠♦# 6 & ♦♠E+&♦ # ♥ &♥&♥ ② # &♦ # R = 1√
2· a
"❮❯ ❨ ❯
!♦♠
❯♥ &( ♣+&, ( ,♥ ♥ ♠& ♠ ② & ♥ ♦ &♥, (♦ ♥ ♥
(7♥ ♦♥ ①&, ♥ ♠♣♦ 9,(♦
~E ( ( ♦, ♣(♠♥ ♥ A(♦ ♥
♥ +♥♦ θ ♥,( (, ② ♦
( ( A ♦,
♣♦♥ A ♦, ♣( ( ♥ ,& α(C · seg−1) ♦
♥( A ♣(♦ &, &( ♣( θ ≪ 1
♦-♥
♦ ♣(♠(♦ A & ( & ,(♠♥( ,♦& & (③& A &,+♥ ,♥♦ &♦(
♦, ② ♦ ,③( ♦♥7♥ A(♦ &♥, ( ♠&,( & (③& A
&,+♥ ,♥♦
♦♥
~FE & (③ ♣(♦ ♣♦( ♠♣♦ 9,(♦ &♦( ( q ② & ♦♠♦
~FE = q ~E
♦♠♦
~E & ♣(♦ X & ,♥(+ A
~E = Ei H♦( ♦ ,♥,♦
~FE = qEi
&(♠♦& ,♥&7♥ ,③♥♦ && ♦♠♣♦♥♥,& (,♥(&
~T = −T sin(θ)i + T cos(θ)j
♦$ & ♣ &♠$ & $③& ♣♦$ ♦♠♣♦♥♥1 ② ♣$ ♦♥4♥ 5$♦
$③ ♥ ❳
∑
FX = qE − T sin(θ) = 0 (1)
$③ ♥ ❨
∑
FY = T cos(θ)−mg = 0 (2)
T =mg
cos(θ)
♠♣③♥♦ ♥
qE − mg
cos(θ)sin(θ) = 0
&1♦ $&1 5
q =mg tan(θ)
E
$&1♦ ♥1$♦$ ♠♦& 1♥♠♦& 5 q = mg tan(θ)E ♦♠♦ θ ≪ 1 1♥♠♦& 5 tan(θ) ≈
θ D♦$ ♦ 1♥1♦ ♣♦♠♦& &$$ $ ♥ ♥4♥ 1♠♣♦ ♦♠♦
q(t) =mgθ(t)
E
$♠♦& ♦♥ $&♣1♦ 1♠♣♦ ♦1♥♠♦&
dq
dt=
mg
E
dθ
dt
♦ ♦♠♦
dqdt = α &♣♥♦ dθ
dt $&1
dθ
dt=
αE
mg
"❮❯ ❨ ❯
!♦♠
♦$ '$ +Q $ ♠♥,♥♥ $ ♥ $,♥ d $♣'3♥ ❯♥ ♣',6 '
♥, −q ② ♠$ m $ $,: ♥ ♥,'♦ $ ② ♦ ,'$ ♥ ♣<=♦ $♣③♠♥,♦
♣'♣♥' 6♥ < $ ♥ $ ♥ ' ♠$,' < ♣',6 $'
♥ ♠♦♠♥,♦ '♠3♥♦ $♠♣ ② ♥♥,' $ ♣'♦♦ ♦$3♥
♦-♥
@' '$♦' ♣'♦♠ ,③' $♥, $♣♦$3♥ $♣
♦ ♣'♠'♦ < ♠♦$ $ ' '③ '$,♥, $♦' ' −q ♦,' < $'
$ '$ $ $♥♦ ♦♣$,♦ ' ♣' $ '③$ $'F♥ ,'②♥,$ ② $'F $,♦
♦ < ♣'♦'F ♦$3♥
♦
~F1
' < ♣'♦ '③
~F1 $ ♥♥,' ♥ ♣♦$3♥ ~r1 = d/2j ② ♣',6
♣' ♥ xi @♦' ♥3♥ '③ ♥,' ♠$ '$ $
~F1 =k(−q)Q(xi + d/2j)
l3
♦
~F2
♥ $, $♦ ' < ♣'♦
~F2 $ ♥♥,' ♥ ♣♦$3♥ ~r2 = −d/2j ♣♦' ♦ ,♥,♦
'③ ,'3♥ ♥,' $, ' ② ' ♣' $'F
~F2 =k(−q)Q(xi− d/2j)
l3
$, ♠♥' '③ '$,♥, $♦' ' −q $'F
~F = ~F1 + ~F2 =−2kqQx
l3i (1)
❱♠♦& ' ♣♦♠♦& +♦♥+ +♦ ℓ ♦♥ & &2♥ d/2 ♥ ♥4♥ 5♥♦ θ ♥♦
♥ + ♥2+♦+ ♣♦+ +4♥ 2+♦♥♦♠72+
d/2
ℓ= cos(θ)
=⇒ ℓ = (d/2) cos(θ)
♦♠♦ & ♣+♦ ♥ ♣':♦ &♣③♠♥2♦ + ♣+ 5♥♦ θ & 2♠7♥
♣':♦ θ ≪ 1 ♦♥ &2♦ ♠♦& ' cos(θ) ≈ 1 ② ♣♦+ ♦ 2♥2♦ ℓ ≈ (d/2) ♥♦ ♥ &
2♥ '
~F =−16kqQx
d3(2)
D♦+ ♣+♠+ ② ♥2♦♥ & 2♥ '
~F = m~a ♥ &2 &24♥ ♣+2F & ♠
&♦+ x ② ♣♦+ ♦ 2♥2♦ m~a = md2xdt2
i &2 ♠♥+ & 2♥+5 '
−16kqQx
d3= m
d2x
dt2
=⇒ d2x
dt2+
16kqQx
md3= 0
♦♥ &2♦ +♠♦& ' + & ♥ ♠♦♠♥2♦ +♠4♥♦ &♠♣ +♥ ♥+
&+5 ♥2♦♥&
w = 4
√
kqQ
md3
♣+♦♦ ♦&4♥ &+5 ♥2♦♥&
T =2π
w=
π
2
√
md3
kqQ
"❮❯ ❨ ❯
!♦♠
♦♥%) %♥. %.)1♥ )% ♣♥.%
♥.♦ ♠♣♦ 7.)♦ ♥ ♣♥.♦ P ♥♦
) ♠♣♦ 7.)♦ ♥ :♠. ♥ ; P %. ♠② ♦ %%.♠
♦.♥
>♦) %♠.): ♠♣♦ 7.)♦ %.)? ♥ )1♥ j ♠♣♦ 7.)♦ ♣)♦♦ ♣♦)
) ♥.) %♦) ♣♥.♦ P %)? %♠♣♠♥.
~E1 =2kq
r2j
♦♠♦ % ? ) % ♦% )% .)% ♣)♦)?♥ ♥ ♠♣♦ 7.)♦ ♥ ♣♥.♦ P ② %
♦♠♣♦♥♥.% ♥ x % ♥)♥ ② ; .♥♥ ) ② %.?♥ %.♥ ♣♥.♦
>♦) ♦ .♥.♦ .♥)♠♦% ; ) ♦♠♣♦♥♥. ♥ y ♠♣♦ ② %♣7% %♠)♦
♣♦) ♣)♥♣♦ %♣)♣♦%1♥ %.♦ % ♣ ) ♥ %♥. )
♦♠♣♦♥♥. ♥ y ♠♣♦ 7.)♦ %)? Ey = E cos(θ) ♠♦♦ ♠♣♦ 7.)♦
E % ♣♦) ♥1♥
E =kq
d2 + r2
♠&' ' & . / cos(θ) = r√
d2+r2 '3 ♠♥. 3♥♠♦' /
Ey = (kq
d2 + r2· r√
d2 + r2)j =
kqr
(d2 + r2)3/2
♦ ♦ / . ' ♥3 ♣♦♠♦' '.. 3♦.♠♥3 '3 ♠♣♦ 3.♦
♦♠♦
~Ey = − kqr
(d2 + r2)3/2j
'3 ♠♣♦ '.& ♣.♦♦ ♣♦. . 3. <♦. ♦ 3♥3♦ ♠♣♦ =3.♦ .'3♥3
♥ ♣♥3♦ P '.& ♣♦. ♣.♥♣♦ '♣.♣♦'>♥
~E = ~Ey + ~Ey + ~E1
♠♣③♥♦ ♦' ♦.' ② ♦3♥♦'
~E = (2kq
r2− 2kqr
(d2 + r2)3/2)j
♥♦ P '3 ♠② ♦ ''3♠ ' 3♥ / d ≪ r ♠♣♦ =3.♦ ♥♦♥3.♦
♥ ♦ ♣♦♠♦' '.. ♦.♠ ♠' . ♦♠♦
~E = 2qk(1
r2− r
(r2 + d2)3
2
)
'3♦ ♦ ♣♦♠♦' '.. ♦.♠ /♥3 ♦♠♦
~E = 2qk(1
r2− 1
r2(1 + d2
r2 )3
2
)
=2qk
r2(1− (1 +
d2
r2)−
3
2 )
♥ ♥. ♥>♥ (1 + x)α' ♣ ♣.♦①♠. ♣♦. 3②♦. ♥♦ x ≈ 0
(1 + x)α = 1 + αx
♦♠♦ d ≪ r ' 3♥ /
dr ≈ 0 ② ♣♦. ♦ 3♥3♦ (d
r )2 ≈ 0 <♦. ♦ 3♥3♦ ♥ ①♣.'>♥
♠♣♦ ♣♦♠♦' . '♥3 ♣.♦①♠>♥
(1 +d2
r2)−
3
2 ≈ (1− 3
2
d2
r2)
♥♦ '3 .'3♦ ♥ ①♣.'>♥ ♦3♥ ♣. ♠♣♦ ' 3♥ /
~E =3qkd2
r4j
"❮❯ ❨ ❯
!♦♠
❯♥ ♣♦♦ *,-♦ ♥ ♥ ♠♣♦ *,-♦ ♥♦-♠ 2 2♣③ -♠♥, 2 ♣♦25♥
6-♦ ♦♠♦ 2 ♠2,- ♥ - ♦♥ θ 2 ♣6:♦ ♠♦♠♥,♦ ♥- ♣♦♦
2 I ♣♦♦ 2 - 2 ♣♦25♥ ♠2,- 6 2 ♦-♥,5♥ ♥- ♣-2♥,
♠♦♠♥,♦ -♠5♥♦ 2♠♣ ② ♥♥,- -♥ ♦25♥
♦-♥
2 -③2 *,-2 6 ,A♥ 2♦- 2 -2 2♦♥ 2 ♥ ♠♥, ② ♥ -5♥ ♣-♦
2,B♥ ♥ 2♥,♦2 ♦♣2,♦2 2,2 -③2 2♦♥ ♥-2 ♣♦- ♠♣♦ *,-♦
~E ② ,♥♥
♠♥, F = qE 2,♦ 2 ♣ ♣-- ♥ 2♥, -
,♦-6 2♦- ♣♦♦ 2-B ♥,♦♥2 2♠ ,♦-62 ♣-♦♦ ♣♦- -③ ♦♥
2-♥♦ -♦,5♥ 2♦- ♣♥,♦ O ♥,♦♥2 2 ,♥-B 6 ,♦-6 2♦- ♣♦♦
2
τ = −Fa sin(θ) +−Fa sin(θ) = −2Fa sin(θ) = −2qE sin(θ)
2♥♦ ♥,♦ 2 ♦,♥ ♣-,- - ♠♥♦ - ② 2 ♣ ♦♠♣-♦-
- ♦♣-♦♥ ♠♦♠♥,♦2 ♦-♠ ,♦-
♠♦2 6 ,♦-6 2♦- ♥ 22,♠ 2-B ♠♦♠♥,♦ ♥- I ♣♦- -5♥
♥- α♠♦2 -2♣,♦ 2♦- O 2 -
τ = Iα
−2qEa sin(θ) = Iα
♦♠♦ 2 ♣-♦♦ 2♦♦ ♥ ♣6:♦ 2♣③♠♥,♦ ♣♦♦ 2 ♠♣ 6 θ ≪ 1 ② ♣♦- ♦
,♥,♦ ♣♦♠♦2 - ♣-♦①♠5♥ sin(θ) ≈ θ ♠B2 ♥♦,♠♦2 6 α = d2θdt2
♠♣③♥♦
2,♦2 ♦-2 ♥ 5♥ ♥,-♦- 2 ,♥ 6
−2qEaθ = Id2θ
dt2
#$ *♥ .♥ ♣♦♠♦# #.. ♦♠♦
d2θ
dt2+
2qEaθ
I= 0
♦♥ ♦ ♠♦# 7 ♦.♥$*♥ ♥. ♣♦♦ #.9 ♥ ♠♦♠♥$♦ .♠*♥♦
#♠♣ ♦♥ .♥ ♥.
w =
√
2qEa
I
❨ ♣♦. ♦ $♥$♦ .♥ #.9
f =w
2π=
1
2π
√
2qEa
I
♣#$♦
♥"%( ♦♦♠
!♦♠
"♥♥ ♦' ♠,' ,♦ ,♦' ♦♥ ♥'' ♥' ♥♦,♠' λ1 λ2 '♣,♦'
♥ '"♥ ,③ 7 ' ,♥ ♠♦' ♠,'
♦-♥ 9♦, ② ♦♦♠ '♠♦' 7 ,③ ;", 7 ①♣,♠♥" ♥ ,
7 ♥ ♣♦'=♥ ~r ♦ ♥ '",=♥ , Ω '
~F = q ·∫
Ω
dq(~r − ~r‘)
4πǫ0|~r − ~r‘|3
9♦♥♠♦' ♠♦' ♠,' ♥ ① " ♦,♠ 7 ♥♦ , x = 0 x = L ②
♦",♦ x = L+d x = 2L+d ♥ ~r1 = x1x ~r2 = x2x ♦♥ 0 ≤ x1 ≤ L ② L+d ≤ x2 ≤ 2L+d
♦' "♦,' ♣♦'=♥ ♠,
♥♠♦' 7 ,③ 7 , '♦, ♥ ♠♥"♦ ① '
~dF21 = dq2 ·∫
Ω1
dq1(~r2 − ~r1)
4πǫ0|~r2 − ~r1|3
= dq2 ·∫ L
0
λ1dx1(x2 − x1)x
4πǫ0|x2 − x1|3
= dq2 ·λ1
4πǫ0· x ·
∫ L
0
dx1
(x2 − x1)2
= dq2 ·λ1
4πǫ0· x · 1
x2 − x1
∣
∣
∣
∣
L
0
=λ1x
4πǫ0· dq2 · (
1
x2 − L− 1
x2)
=λ1λ2x
4πǫ0· dx2 · (
1
x2 − L− 1
x2)
"❮❯ ❯
=⇒ ~F21 =λ1λ2x
4πǫ0·∫ 2L+d
L+d
(
1
x2 − L− 1
x2
)
dx2
=λ1λ2x
4πǫ0· (ln(x2 − L)− ln(x2))|2L+d
L+d
=λ1λ2x
4πǫ0· ln(
x2 − L
x2)
∣
∣
∣
∣
2L+d
L+d
=⇒ ~F21 =λ1λ2
4πǫ0· ln
(
(L + d)2
d(2L + d)
)
· x
❨ $% $ *③ ,%* / $ *♥ ♠♦$ ♠*$ ♣$ $♠♦$ / ② ♦♦♠
$%$ * ② %=♥ ♦*♠ *%
!♦♠
♠' ' -. ♦'♠♦ ♣♦' ♥ ♣'. -♠'' BCD '♦ R❬♠❪ ② ♣♦'
♦- '.9♥- ♦♥.- AB = 2R ❬♠❪ ② DE = R ❬♠❪ ♦- '♦- BC ② CD -.<♥ ♥
♦'♠♠♥. '♦- ♦♥ '- q ② −q '-♣.♠♥. ♠♥.'- A -♦' AB .♠B♥
- -.'② ♥♦'♠♠♥. ♥ ' q ♥. ' '♣'.'- ♦♥ ♥-
♦♥-.♥. -♦' .'③♦ DE ♣' A ♠♣♦ B.'♦ - ♥♦ ♥ ♥.'♦ O
♦♦♥
♦ A '♠♦- -'< ' ♠' ♦♠♣.♦ ♥ ♣'.- . ♦♠♦ ♠-.' '
'♠♦- ♠♣♦ .'♦ ♣'♦♦ ♣♦' - '♦♥- ♥ O ② ♦ ♦- -♣'♣♦♥'♠♦-
♠♣♦♥'♠♦- ♦♥♦♥ A ♠♣♦ .'♦ ♥ -. '♦♥ - ♥♦
!♦③♦
♠' - '.♥♦ ② '♦ 2R ② .♥ ♥ ♥ ' q ♥♦'♠♠♥. -.'
-. ♠♥' ♣♦♠♦- ♥' - ♥- ' ♦♠♦ λ1 = q2R
-. ♠♥' - .♦♠♠♦-
♥ ♣AJ ' dq ♠' -♠♦- A - ♠♣ '♦♥ dq = λ1dx ♦♥ dx -
♥ ♣AJ♦ .'♦③♦ ♠'
♠♣♦ .'♦ A ♣'♦ ♠♥.♦ dq -.' ♥ '♦♥ i ♣♦' ♦ .♥.♦ ♠♣♦
.'♦ A ♣'♦ -'<
"❮❯ ❯
d ~E1 = (kdq
x2)i = (
kλ1dx
x2)i
♥#&♥♦ * x = −3R *# x = −R
~E1 = k(λ1
∫
1
x2dx)i = (kλ1(−
1
x2
∣
∣
∣
∣
−R
−3R
))i
♦ - &*#
~E1 =2kλ1
3Ri
" &♦ ♦& "♦& )♥"♠♦& , &♣"♣♦♥"♥♦& ♠♣♦ )"♦ "&)♥) &)"
♥ "♦♥ hati &)♦ , ♥♠♥)♠♥) "♦ " &♥) "
♦♠♦ ♠♦& "♦ BC )♥ " ♣♦&) ♥ ② ♣♦" ♦ )♥)♦ ♠♥)♦ "
♥" ♥ ♠♣♦ &♥) ♠&♥)"& , "♦ CD )♥ " ♥) ② ♠♥)♦
" ♥" ♥ ♠♣♦ ♥)"♥) &) ♠♥" ♦ , ♠♦& " & &♠♣♠♥)
" & ♦♠♣♦♥♥)& ♥ x ♠♣♦ ② &♣& &♠"&
& ♥&& " ♣" "♦ & ♦)♥♥ ♠♥) &" , )♥ ♣♦&)
♥ " , ② , ② )♥♥ ♥ "♦
πR2
λ2 =2q
πR
λ3 = − 2q
πR
!♦ ♦♥&"♠♦& ♥ ♣,? " dq "♦ ♠♦♦ ♠♣♦ )"♦ ♣"♦
♦ ♣♦" &) " &"@ &♠♣♠♥)
dE =kdq
R2
♦♥ ② ♥& " λ2 ♣♦♠♦& &"" dq = λ2ds ♦♥ ds & ♥ ♣,?♦
)"♦③♦ "♦ &) )"♦③♦ "♦ ♦ ♣♦♠♦& &"" ♥ ♥♦♥ ♥♦ , ♦ "♦""
ds = Rdθ
"♦♠♦' ♥)♦♥' '++ ♠♣♦ ♦♠♦
dE2 =kλ2Rdθ
R2=
kλ2dθ
R
♦ ♦♠♣♦♥♥) ♥ x ♠♣♦ dE2 '+
dEx2 = dE2 cos(θ) =kλ2 cos(θ)dθ
R
♥)+♥♦ ' θ = 0 ') θ = π2
Ex2 =kλ2
R
∫ π
2
0cos(θ)dθ =
kλ2
R
❱)♦+♠♥)
~Ex2 =kλ2
Ri
!♦ ♦ ' + ♦♠♣♦♥♥) ♥ x ♠♣♦ ♣+♦♦ ♣♦+ ') +♦ '+<
♥)+♦+ ') ♠♥+
~Ex3 =kλ2
Ri
' ' )♥+ >
~E2 + ~E3 = 2kλ2
Ri
!♦③♦
q′ + > )♥ ') )+♦③♦ ♠+ ) > ♥ ♠♣♦ )+♦ ♣+♦♦
♣♦+ )♦♦ ♠+ ♥ O ♦♠♦ )♥ +♦ R ♥' + '+<
λ4 =q′
R
♦ ♣+♦♥♦ ♦+♠ > ♣+ )+♦③♦ AB ♠♦' >
~E4 = (kλ4
∫ 2R
R
1
x2dx)i = (
−kλ4
2R)i
♠♥♦ )♦♦' ♦' ♠♣♦' ♦' ♥♦ +♦
~E1 + ~E2 + ~E3 + ~E4 =2kλ1
3Ri +
2kλ2
Ri + (
−kλ4
2R)i = 0
"❮❯ ❯
$♣♥♦ λ4
λ4 =2
3(2λ1 + 6λ2)
♠♣③♥♦ ♦$ ♦1$ λ1 λ2 ② λ4 ♥♦$ ♥61♦1♠♥6 ♥♦♥61♠♦$ ♦1
1 $
q′ =2
3q(1 +
12
π)
♦♥$1♠♦$ π ≈ 3
q′ =10
3q
!♦♠
♠♣♦ +,-♦ ♣-♦♦ ♣♦- ♥ ♣♥♦ ♥♥,♦ ♥2 - ♥♦-♠ σ
♦-♥
♦♥2-♠♦2 ♣♥♦ ♥ 2,6♥ ♣♥♦ ①② ♦♦-♥2 -,2♥2 ♠♦2 ;
♠♣♦ +,-♦ ♥ ♦ ♣♦-
~E(~r) =
∫ ∫
Ω
dq(~r − ~r1)
4πǫ0|~r − ~r1|3
♦♥ ~r1 ,♦- ♣♦26♥ 2,-6♥ - Ω ; ♥- ♠♣♦ +,-♦ ♥ ~r
♥♠♦2 ; ~r = xx + yy + zz ~r1 = x1x + y1y ② |~r − ~r1|2 = (x− x1)2 + (y − y1)
2 + z2
=⇒ ~E(~r) =
∫ +∞
−∞
∫ +∞
−∞
σdx1dy1((x− x1)x + (y − y1)y + zz)
4πǫ0((x− x1)2 + (y − y1)2 + z2)3
2
♠♦2 ♠♦ -2 w = x − x1 v = y − y1 =⇒ x1 = x − w, y1 = y − v
♦♥♦ ,-♥2♦-♠6♥ 2
J =
∣
∣
∣
∣
(x1)w (x1)v
(y1)w (y1)v
∣
∣
∣
∣
=
∣
∣
∣
∣
−1 00 −1
∣
∣
∣
∣
= 1
=⇒ ~E(~r) =
∫ +∞
−∞
∫ +∞
−∞
σdwdv(wx + vy + zz)
4πǫ0(w2 + v2 + z2)3
2
=σ
4πǫ0
∫ +∞
−∞
∫ +∞
−∞
dwdv · (zz)
(w2 + v2 + z2)3
2
♠♥, ♠♦2 ♠♦ -2
w = rcos(θ)
v = rsen(θ)
J =
∣
∣
∣
∣
wr wθ
vr vθ
∣
∣
∣
∣
=
∣
∣
∣
∣
cos(θ) −rsen(θ)sen(θ) rcos(θ)
∣
∣
∣
∣
= r
=⇒ ~E(~r) =σ
4πǫ0
∫ 2π
0
∫ +∞
0
rdrdθ · (zz)
(r2 + z2)3
2
=σ
4πǫ0· 2πzz
∫ +∞
0
rdr
(r2 + z2)3
2
pero u = r2 + z2 → du = 2rdr
=σ
4ǫ0· zz
∫ +∞
z2
du
(u)3
2
=σ
4ǫ0· zz
(
2u−1
2
)∣
∣
∣
z2
+∞
=σ
2ǫ0· z
|z| z
=σ
2ǫ0· sign(z)z
!♦♠ ♦♥%) ♥ ♣♥♦ ♥♥/♦ ♥% ) ♥♦)♠ σ ♦♥ ♥ ♦)♦
)) )♦
♠♣♦ 8/)♦ ♥ 9) ♣♥/♦ 9 ♣% ♣♦) ♥/)♦ ♦)♦
♣)♣♥)♠♥/ ♣♥♦
♦ )♦ % ♦♦ ♥ ♠) ♥♦ ♦♥/♦) )♦ ♦♥ ♥%
) ♥ ♥♦)♠ λ ② ② %/♥ ♠?% ♣)@①♠ ♣♥♦ % ♥♦♥/)) )③
8/) 9 ①♣)♠♥/ ♠)
♦.♥
❯%♥♦ ♣)♥♣♦ %♣)♣♦%@♥ ♣♦♠♦% ♥♦♥/)) ♦ %♦ ♦♥%)♥♦
%♠ /♦) ♠♣♦ 8/)♦ 9 ♥) ♥ ♣♥♦ ♥♥/♦ ♥% ) σ
%♦) ② ♥ %♦ )♦ ② ♥% ) −σ ♣♥♦ ②③ ♦♦)♥♦
♣♥♦ ♥ %/@♥ ② ① ♥ %/@♥
♦% /♠% ♥/)♦)% /♥♠♦% 9 ♠♣♦ 8/)♦ ♥)♦ ♣♦) ♣♥♦ %
~E1(~r) =σ
2ǫ0· sign(x)x
② ♠♣♦ 8/)♦ ♥)♦ ♣♦) %♦ %
~E2(~r) =−σ
2ǫ0· x(
sign(x)− x√R2 + x2
)
=⇒ ~E = ~E1 + ~E2 =σ
2ǫ0·(
x√R2 + x2
)
x
♥♠♦% 9 )③ 8/) 9 ①♣)♠♥/ ♥ ♠♥/♦ dx ♠) ♦
"❮❯ ❯
♣♥♦ ♦♥ ♦)♦ ,-. ♣♦) d~F = dq ~E
=⇒ ~F =
∫ d+a
d
dq ~E con dq = λdx
=
∫ d+a
d
λdxσ
2ǫ0·(
x√R2 + x2
)
x
=λσ
2ǫ0·∫ d+a
d
xdx√R2 + x2
· x
=λσ
2ǫ0·(√
R2 + x2)∣
∣
∣
d+a
d· x
=λσ
2ǫ0·(
√
R2 + (d + a)2 −√
R2 + d2)
· x
!♦♠
❯♥ $♣♥) *♠♠*$♦ ♥♦ ♦♥)♦$ $♦ a )♥ ♥ $ )♦) Q ♥♦$♠♠♥)
*)$ ♥ * *♣$ ♥)$♦$ ♥♥)$ ♠♣♦ 8)$♦ ♥ ♣♥)♦ O
♦.♥
*) ♣$♦♠ ♦ ♠♦* $*♦$ )③♥♦ ② ♦♦♠ ♣$ *)$♦♥* *♣$
* $ *) ② ♥♦* ♣$ *) *♦ =
~E(~0) =
∫
kdq(~r − ~r′)
‖~r − ~r′‖3
♦♠♦ ② ♠♦* *)♦ ♠♥)♦ $ ♦ ♣♦♠♦* *$$ ♦♠♦ dq = σdA ♦♥ σ *
♥* $ *♣$ ♥ ♥)$♦$ $♣♥) ♦♥*)♥) ♠♦* *$$
♠♥)♦ C$ dA ) ♠♥$ = ♣♦♠♦* $♦$$$ *♣$ ② ♣$ *)♦ $♠♦* ♦
*♥) ♦♥*$$ ♥ *$ *8$ ♦♥ *♥) *♣♦*E♥ ♣$ * $* θ ②
γ
$ ♥ ♣=G $E♥ C♥♦ θ ♠♦* = * $♦$$ ♥ ♣=G♦ $♦ ♦♥)
ds1 = R sin(γ)θ H♦$ ♦)$♦ ♦ $ ♥ ♣=G $E♥ C♥♦ γ * $♦$$ ♥ $♦
♦♥) ds2 = Rdγ *) ♠♥$ ♠♥)♦ C$ $♥$♥ ♦ ♣♦♠♦*
*$$ ♦♠♦
dA = ds1 · ds2 = R2 sin(γ)dγdθ
*) ♠♥$ ♣♦♠♦* *$$ ♠♥)♦ $ ♦♠♦
dq = σR2 sin(γ)dγdθ
"❮❯ ❯
"♦$ ♦%$♦ ♦ ♠♦- %$♠♥$ ♦- %♦$-
~r′ ② ~r $♠♥%
~r′ = ~0 ② ♣♦$ ♦%$♦
♦♠$♥♦ $ $♠♦- <
~r = R sin(γ) cos(θ)i + R sin(γ) sin(θ)j + R cos(γ)k
♦ - ? $ < ‖~r − ~r′‖ = R
-% ♠♥$ -♣♥♦ ♦- $♦$$♦- - $- ♣$ < $♦$$♥ $♣♥% -
%♥ <
~E(~0) =
∫ 2π
0
∫ 3π
2
π
2
kσ(−R sin(γ) cos(θ)i−R sin(γ) sin(θ)j −R cos(γ)k)
R3R2 sin(γ)dγdθ
"♦$ -♠%$? -♠♦- < ♠♣♦ A%$♦ $-%♥% -%$B ♥ $C♥ k ② ♣♦$ ♦ %♥%♦
♥%$ ♥%$♦$ ♥♦ ♦♥-$♠♦- - ♦♠♣♦♥♥%- $-%♥%-
~E(~0) =
∫ 2π
0
∫ π
π
2
kσ(− cos(γ)k) sin(γ)dγdθ = kσ
∫ 2π
0dθ
∫ π
π
2
(− cos(γ)k) sin(γ)dγ = πkσ
∫ π
π
2
(− sin(2θ)k))dγ
-% ♠♥$
~E(~0) = πkσ(1
2cos(2θ)
∣
∣
∣
∣
π
π
2
)k = πkσ1
2(cos(2π)− cos(π))k = (πkσ)k
♥♠♥% ♣$ -$$ -% $-%♦ ♥ ♥C♥ Q ♠♦- %$♠♥$ ♦$ σ
-%♦ - B -♥♦ < $ -% ♥♦$♠♠♥% -%$ ♥ -♣$ ♥%$♦$
%♥$♠♦- <
σ =Q
2πR2
-% ♠♥$
~E(~0) =kQ
2R2k
!♦♠
♥ ) ♠) AB .♥ ♦♥. 2L ② 3 ♣)♣♥) ♠) CD ♦♥.
L ♥♦ ♦3 .♥ ♠3♠ ) Q 3.) ♥♦)♠♠♥. ♠♥.
② )9♥ )③ ; ♥♦ ♦3 ) 3♦) ♦.)♦
♦.♥
3. ♣)♦♠ 3 )3 ♦)♠ ; ♣)♦♠ ♥.)♦) ♦ ♣)♠)♦ ; )♠♦3
3 ) ♠♣♦ @.)♦ ; ♣)♦ ♠) ). 3♦) ♥ ♣♥.♦ 3
3♠.)A ♦♠♦ ) Q 3. ♥♦)♠♠♥. 3.) 3 .♥)B ; 3♦) ♠♣♦
@.)♦ 3.)B ♥ )9♥ j
♠♣♦ @.)♦ ♣)♦♦ ♣♦) ♥ ) dq 3)B dE = kdqr2 ♦♥ r 3 3.♥ 3
) dq ♥ xi 3. ♣♥.♦ ♣9♥ dj r =√
x2 + d2 ♦♠♦ ♦
♠♦3 ♦ ♥.3 ) dq ♣♦♠♦3 3)) ♦♠♦ dq = λ1dx ♦♥ λ1 3 ♥3
♥ ) ② ♥♠♦3 ♦♠♦ λ1 = Q2L
3 ♠♣♦ ; ①♣)3♦ ♦♠♦
dE =kλ1dx
x2 + d2
❨ ♠♦3 ; ♠♣♦ 3.)B ♥ )9♥ j ② ; 3 ♦♠♣♦♥♥.3 ♥ x 3 ♥)♥ 3
♦♠♣♦♥♥.3 ♥ y 3 ♣♦♠♦3 3)) ♦♠♦ dEy = dE cos(θ) 3 ) ;
cos(θ) =d
√
(x2 + d2)
"❮❯ ❯
$% ♠♥)
dEy =kλ1ddx
(x2 + d2)3
2
♥%)♥♦ $ x = −L $% x = L
Ey = kλ1d
∫ L
−L
1
(x2 + d2)3
2
dx = kλ1d(x
(d2√
x2 + d2
∣
∣
∣
∣
L
−L
) =2kλ1L
d√
L2 + d2
$% ♠♥) )③ 4 ) ♠) ♦)③♦♥% $♦) ♥ ♣4: ) dq
♠) )% 4 $% ♥ %) y $)<
dF = dqE = dq2kλ1L
d√
L2 + y2
$% ♠) %♥ $%♥% ♥$ ) ② 4 $ ♥ %♥ ♠$♠ ) %♦% ♠
♥ %♥ ♠% )♦ 4 ♠) ♦)③♦♥% $% ♠♥) ♥♠♦$
λ2 =Q
L
$ dq = λ2dy ② )③ 4 ①♣)$ ♦♠♦
dF = λ2dy2kλ1L
y√
L2 + y2
♥%)♥♦ $ y = L $% y = 2L
F = 2kλ1λ2L
∫ L
−L
1
y√
L2 + y2dy
%♥ 4
∫
1
y√
L2 + y2dy =
1
Lln(
√
L2 + y2 − L
y)
F♦) ♦ %♥%♦
F = 2kλ1λ2L(1
Lln(
√
L2 + y2 − L
y)
∣
∣
∣
∣
∣
2L
L
)
$))♦♥♦
F = 2kλ1λ2 ln(
√5− 1
2(√
2− 1))
♠♣③♥♦ ♦$ ♦)$ λ1 ② λ2 ♥ ♥H♥ Q
F =kQ2
L2ln(
√5− 1
2(√
2− 1))
!♦♠
(③ ♣♦" ♥ "♦ * + (♥ ♥ ♥ ♥♥1♠♥1 ( ♥♦ b
② ♥+ ( ♥♦(♠ σ ② ♥ ♠( ♠♥1 (♦ ♦♥ ♥+ ( ♥♦(♠
λ ♣+1♦ ♥ ♠+♠♦ ♣♥♦ * ♥ ♥ +1♥ d
♦.♥
♦♠♦ (③ ♦♦♠ ♠♣ ( ② 1=♥ (♠♦+ ♦(♠ ♠>+ +♠♣
( (③ ♣♦( ♥ (♦ * + (♥ ♠♦+ ♦1♦+ +1♦ + (③ ♥♦
♦1(♦ +♦( ♦1(♦ A♦♥♠♦+ ♠( ♥ ① ② + ♣♥♦ ♦♥ +1>♥ ♠♦+ ♦1♦+
♣♥♦ ①② +♠1(D ♣(♦♠ ♠♦+ * (③ * ( ♥ +♦( ♥
♠♥1♦ ① ♠( +1> ( ♥ ±y ② + ♠+♠ ♥ *( ♣♥1♦ ♠(
A♦( 1♥1♦ ♥♦+ +1 ( (③ ♣♦( ♥ (♦ ♥ ① ♠(
♥ ~r2 = ~0 ~r1 = xx + yy ♦♥ −∞ ≤ x ≤ +∞ ② d ≤ y ≤ b + d ♣♦+=♥ ♠♥1♦ ①
♥ ① ♠( ② ♣♦+=♥ ♥ (+♣1♠♥1 +D 1♥♠♦+ * (③
+♦( 1 ♠♥1♦ +
~dF21 = dq2
∫ ∫
Ω
dq1 · −~r1
4πǫ0|~r1|3, con dq1 = σdxdy
= −dq2
∫ +∞
−∞
∫ b+d
d
σdxdy · xx
4πǫ0(x2 + y2)3
2
− dq2
∫ +∞
−∞
∫ b+d
d
σdxdy · yy
4πǫ0(x2 + y2)3
2
= −dq2σy
4πǫ0
∫ +∞
−∞
∫ b+d
d
dxdy · y(x2 + y2)
3
2
=dq2σy
4πǫ0
∫ +∞
−∞
(
1√
x2 + y2
)∣
∣
∣
∣
∣
b+d
d
· dx
=dq2σy
4πǫ0
∫ +∞
−∞
(
1√
x2 + (b + d)2− 1√
x2 + d2
)
· dx, pero dq2 = λdx2
=⇒~dF21
dx2=
λσy
4πǫ0
∫ +∞
−∞
(
1√
x2 + (b + d)2− 1√
x2 + d2
)
· dx
=λσy
2πǫ0· ln
(
x +√
x2 + (b + d)2
x +√
x2 + d2
)∣
∣
∣
∣
∣
+∞
0
=λσy
2πǫ0·
lımx→+∞
ln
1 +
√
1 + ( b+dx
)2
1 +
√
1 + ( dx)2
− ln
(
b + d
d
)
=λσy
2πǫ0· ln
(
d
b + d
)
=⇒~dF21
dx2=
λσy
2πǫ0· ln
(
d
b + d
)
"❮❯ ❯
!♦♠
♦♥%) ♥ ♠) )01♥♦ ♥♥0♦ ♥ %0♥ R ♥ ♠) %♠)) )♦
R ♦♠♦ % ♥ ) ♠♦% %07♥ ♥♦)♠♠♥0 )♦% ♦♥ ♥% ♥ )
λ ♥♥0) )③ )♣%<♥ ♥0) ♠%
♦.♥
♦ ♣)♠)♦ > ♠♦% % ) ♠♣♦ @0)♦ ♣)♦♦ ♣♦) ♥ ♠) ♥♥0♦ ♥
%0♥ d @ ♠♣♦ @0)♦ 0♥)7 )<♥ j ② > %) ♠) ♥♥0♠♥0
)♦ % ♥)♥ % ♦♠♣♦♥♥0% ♠♣♦ ♥ x %0♦ % ♣ ♣)) ♥ %♥0 )
♦♠♣)♦♠♦% %0♦ ♥♦ ♠♣♦ ♠♣♦ @0)♦ > ♣)♦ ♥ ♣>C )
dq ♥ ♣♥0♦
~r′ = xi ♠) %♦) ♣♥0♦ ~r = dj %)7
d ~E =kdq(~r − ~r′)
|~r − ~r′|3=
kdq(−xi + dj)
(x2 + d2)3
2
♦) % 0♥ > dq = λdx ② ♣♦) ♦ 0♥0♦
d ~E =kλdx(−xi + dj)
(x2 + d2)3
2
♥0)♥♦ % −∞ +∞
~E =
∫ +∞
−∞
kλdx(−xi + dj)
(x2 + d2)3
2
= kλ((−∫ +∞
−∞
x
(x2 + d2)3
2
)i + (
∫ +∞
−∞
d
(x2 + d2)3
2
)j)
♥)♥ f(x) = x
(x2+d2)3
2
+ ♠♣. ② ♣♦. ♦ 2♥2♦ ♥2. +2 ♥)♥ ♥ ♥ ♥2.♦
♣. 2♦♠ ♦. 8♦. ♦2.♦ ♦ ♥)♥ g(x) = d
(x2+d2)3
2
+ ♣. ② ♥2. +2 ♥)♥
+ −∞ +∞ +.: ♦ ♥2. ① + +∞
∫ +∞
−∞
g(x)dx = 2
∫ +∞
0g(x)dx
8♦. ♦ 2♥2♦ ①♣.+)♥ ♣. ♠♣♦ + .
~E = 2kdλ
∫ +∞
0
1
(x2 + d2)3
2
j
2♥ A
∫
1
(x2+d2)3
2
= x
d2(x2+d2)1
2
8♦. ♦ 2♥2♦
~E = 2kdλ(x
d2(x2 + d2)3
2
∣
∣
∣
∣
∣
∞
0
)j =2kλ
dj
♦. A +♠♦+ ♦♠♦ + ♠♣♦ D2.♦ ♥.♦ ♣♦. ♥ ♠. ♥♥2♦ ♣♦♠♦+
. .③ +♦. ♠. +♠.. 8. . +2 .③ ♦♥+..♠♦+ ♣AH♦+
2.♦③♦+ ♦♥ . dq ♥ .③ ♣ +♦. +.: ♣♦. ♥)♥dF = dqE
♦♥ E + ♠♣♦ D2.♦ ♣.♦♦ ♣♦. ♠. ♥♥2♦ 2. ♥ A + ♥♥2.
. dq ♦...D ♦+ ♠♥2♦+ . ♠. ♥ ♥)♥ ♥ :♥♦ θ A .♦..
♠. +♠.. ♦♥+.. +♥2 .
♠♣♦ D2.♦ ♣.♦♦ ♣♦. ♠. ♥♥2♦ ♣♥ +2♥ + +2
♦♠♦ 2. ♠♥2♦ dq . . .③ ♣.♦ +♦. ♥
+2+ .+ 2♠D♥ ♦ .: 2. ♠♥2♦ dq ♥ ♥)♥ :♥♦ θ A
①♣.+ ♦♠♦ d(θ) = R + R sin(θ) ♠:+ ♠♥2♦ . dq + ♣♦. ♥)♥
λds ♦♥ ds + ♥ ♣AH♦ 2.♦③♦ ♠. .. ♣♦♠♦+ +.. ♥ ♥)♥
:♥♦ θ ♦♠♦ ds = Rdθ +2 ♠♥. .③ +♦. ♥ . dq +.:
dF = dqE = λRdθ · 2kλ
R + R sin(θ)=
2kλ2dθ
1 + sin(θ)
♥2.♥♦ + θ = 0 θ = π ♦2♥♠♦+ .③ 2♦2 +♦. ♠. +♠.. 8.
+2♦ 2③♠♦+ ♦ A