PH2200 Formula Sheet - Physics
PH2200 Formula Sheet - Physics
PH2200 Formula Sheet - Physics
You also want an ePaper? Increase the reach of your titles
YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.
<strong>PH2200</strong> <strong>Formula</strong> <strong>Sheet</strong><br />
Electric Fields<br />
! kqq e 1 2 1<br />
F ˆ<br />
12<br />
= r k<br />
2<br />
e<br />
=<br />
r<br />
4πε<br />
o<br />
!<br />
! Fe<br />
E = lim<br />
qo<br />
→0<br />
qo<br />
! kq e<br />
E = rˆ<br />
2<br />
r<br />
! " kq<br />
E = E = rˆ<br />
∑<br />
∑<br />
e i<br />
i<br />
2 i<br />
i i ri<br />
! " kdq e<br />
E = ∫dE = ∫ rˆ<br />
2<br />
r<br />
Gauss's Law<br />
! !<br />
Φ = E⋅dA<br />
# ∫<br />
E<br />
! ! qin<br />
E⋅ dA=<br />
ε<br />
σ<br />
E =<br />
ε<br />
°<br />
∫<br />
°<br />
at conductor surface<br />
Electric Potential<br />
B ! !<br />
∆ U =−q E⋅ds<br />
kq e<br />
V()<br />
r =<br />
r<br />
kq e i<br />
V = ∑<br />
r<br />
x<br />
i<br />
12<br />
o<br />
i<br />
A<br />
B<br />
∆U<br />
! !<br />
∆ VA→B<br />
= =− E⋅ds<br />
q<br />
∫<br />
kdq e<br />
V = ∫<br />
r<br />
kqq e 1 2<br />
U =<br />
r<br />
E<br />
dV<br />
=−<br />
dx<br />
∫<br />
o<br />
Capacitance and Dielectrics<br />
Q<br />
C = ∆ V<br />
ε A<br />
C = °<br />
parallel-plate capacitor<br />
d<br />
A<br />
C 1<br />
= cylindrical capacitor<br />
l ⎛b<br />
⎞<br />
2ke<br />
ln⎜<br />
⎟<br />
⎝a<br />
⎠<br />
ab<br />
C =<br />
spherical capacitor<br />
k ( b − a )<br />
e<br />
C = C + C + C + ... parallel<br />
eq<br />
1<br />
2<br />
1 2 3<br />
1 1 1 1<br />
= + + + ... series<br />
C C C C<br />
eq<br />
1 2 3<br />
2<br />
Q<br />
1 1<br />
U = =<br />
2Q∆ V =<br />
2C( ∆V)<br />
2C<br />
2<br />
u = ε E<br />
E<br />
C = κC<br />
°<br />
o<br />
Current and Resistance<br />
∆Q<br />
Iav<br />
= ∆ t<br />
dq<br />
I =<br />
dt<br />
Iav<br />
= nqvd<br />
A<br />
! !<br />
J = nqvd<br />
! !<br />
J = σ E<br />
∆V<br />
R =<br />
I<br />
1<br />
ρ = σ<br />
ρl<br />
R =<br />
A<br />
ρ = ρ [1 + α( T −T<br />
)]<br />
o<br />
P = I∆V<br />
2 ( ∆V<br />
)<br />
P = I R=<br />
R<br />
Direct Current Circuits<br />
2<br />
R = R + R + R + ... series<br />
eq<br />
1 2 3<br />
1 1 1 1<br />
= + + + ... parallel<br />
R R R R<br />
eq<br />
∑Iin<br />
∑<br />
=<br />
closed loop<br />
o<br />
1 2 3<br />
∑<br />
I<br />
out<br />
∆ V = 0<br />
2<br />
qt = CE<br />
−e<br />
−t/<br />
RC<br />
( ) (1 ) charging<br />
It<br />
E<br />
= e<br />
R<br />
qt = Qe<br />
−t/<br />
RC<br />
( ) charging<br />
−t/<br />
RC<br />
( ) discharging<br />
Q<br />
=− e<br />
RC<br />
−t/<br />
RC<br />
( ) discharging<br />
It<br />
Magnetic Fields<br />
! ! !<br />
F = qv×<br />
B<br />
B<br />
FB<br />
= q vBsinθ<br />
! ! !<br />
FB<br />
= I L×<br />
B<br />
! ! !<br />
dFB<br />
= Ids × B<br />
! !<br />
µ = NIA<br />
! ! !<br />
τ = µ × B<br />
! !<br />
UB<br />
=−µ<br />
⋅B<br />
! ! ! !<br />
F = qE + qv×<br />
B<br />
mv qB<br />
r = , ω =<br />
qB m<br />
Sources of the Magnetic Field<br />
!<br />
!<br />
µ<br />
o Ids × rˆ<br />
dB =<br />
2<br />
4π<br />
r<br />
µ<br />
oI<br />
B = long straight wire<br />
2π<br />
a<br />
FB<br />
µ<br />
oII<br />
1 2<br />
=<br />
l 2π<br />
a<br />
! !<br />
B⋅ ds = µ I<br />
# ∫<br />
µ<br />
oNI<br />
B =<br />
2π<br />
r<br />
N<br />
B= µ<br />
o I = µ<br />
onI<br />
l<br />
! !<br />
Φ<br />
B<br />
= ∫ B⋅dA<br />
! !<br />
B⋅ dA=<br />
0<br />
# ∫<br />
Faraday's Law<br />
dΦ<br />
E =−N<br />
dt<br />
E =−Blv<br />
o<br />
B<br />
dΦ<br />
∫ E ! !<br />
# ⋅ ds =−<br />
dt<br />
B<br />
toroid<br />
solenoid
Inductance<br />
dΦ<br />
E<br />
dt<br />
NΦB<br />
L =<br />
I<br />
2<br />
µ<br />
oN A<br />
L =<br />
l<br />
E<br />
I = −e<br />
R<br />
E −Rt / L<br />
I = e<br />
R<br />
2<br />
U = LI<br />
B<br />
L<br />
=− N =−<br />
1<br />
2<br />
dI<br />
L<br />
dt<br />
−Rt / L<br />
(1 ) rising current<br />
2 12 1 21<br />
12 21<br />
I1 I2<br />
solenoid<br />
decaying current<br />
2<br />
B<br />
uB<br />
=<br />
2µ<br />
°<br />
N Φ N Φ<br />
M = = M = = M<br />
dI<br />
dI<br />
E =− M and E =−M<br />
dt<br />
dt<br />
Q= Qmax<br />
cos( ωt+<br />
φ)<br />
1<br />
ω =<br />
LC<br />
U = UC<br />
+ UL<br />
2 2<br />
Qmax<br />
2 LImax<br />
2<br />
= cos ωt+<br />
sin ωt<br />
2C<br />
2<br />
1 2<br />
2 12 1 21<br />
Alternating Current Circuits<br />
Irms<br />
= 0.707I<br />
∆Vrms<br />
0.707V<br />
X = ωL<br />
L<br />
1 1 2 2<br />
max<br />
max<br />
1<br />
X C<br />
=<br />
ωC<br />
2 2<br />
Z = R + ( XL<br />
− XC)<br />
−1<br />
⎛ XL<br />
− XC<br />
⎞<br />
φ = tan ⎜ ⎟<br />
⎝ R ⎠<br />
Pav = Irms∆Vrms<br />
cosφ<br />
2<br />
Pav<br />
= IrmsR<br />
∆Vrms<br />
Irms<br />
=<br />
R + ( X − X )<br />
1<br />
ωo<br />
=<br />
LC<br />
I ∆ V = I ∆V<br />
2 2<br />
L C<br />
Electromagnetic Waves<br />
# ∫<br />
S<br />
# ∫<br />
S<br />
! ! Q<br />
E⋅ dA=<br />
εo<br />
! !<br />
B⋅ dA=<br />
0<br />
! ! dΦ<br />
B<br />
# ∫ E⋅ ds =−<br />
dt<br />
! !<br />
dΦ<br />
# ∫ B⋅ ds = µ<br />
oI<br />
+ ε<br />
oµ<br />
o<br />
dt<br />
1<br />
c =<br />
εµ<br />
o o<br />
fλ<br />
= c<br />
Emax<br />
E<br />
= = c<br />
Bmax<br />
B<br />
! !<br />
! E×<br />
B<br />
S =<br />
µ<br />
°<br />
E B<br />
= = =<br />
max max<br />
I Sav<br />
cuav<br />
2µ<br />
o<br />
2<br />
1 2 B<br />
uB = uE = ε<br />
2 oE<br />
=<br />
2µ<br />
o<br />
B<br />
u = ε E =<br />
av<br />
1<br />
2<br />
o<br />
2<br />
2 max<br />
max<br />
2µ<br />
o<br />
U S<br />
p= P=<br />
c c<br />
2U<br />
2S<br />
p = P =<br />
c c<br />
E<br />
complete absorption<br />
complete reflection<br />
The Nature of Light and<br />
the Laws of Geometric Optics<br />
θ'<br />
1<br />
= θ1<br />
n1sinθ1 = n2sinθ2<br />
c<br />
n =<br />
v<br />
λ<br />
λn<br />
=<br />
n<br />
n<br />
θ = ><br />
2<br />
sin<br />
c<br />
(for n1 n2)<br />
n1<br />
Geometric Optics<br />
h'<br />
M =<br />
h<br />
1 1 2 1<br />
+ = =<br />
p q R f<br />
n n n − n<br />
+ =<br />
p q R<br />
1 2 2 1<br />
1 ⎛ 1 1 ⎞<br />
= ( n −1)<br />
⎜ − ⎟<br />
f ⎝ R1 R2<br />
⎠<br />
1 1 1<br />
+ =<br />
p q f<br />
Physical Constants<br />
9 2 2<br />
ke<br />
= 8.988× 10 N⋅m / C<br />
−12 2 2<br />
εo<br />
= 8.854× 10 C / N⋅m<br />
−19<br />
e= 1.602 × 10 C<br />
−31<br />
melectron<br />
= 9.109 × 10 kg<br />
−27<br />
mproton<br />
= 1.672×<br />
10 kg<br />
−7<br />
µ<br />
°<br />
= 4π<br />
× 10 T⋅m/<br />
A<br />
1<br />
8<br />
c= = 2.998×<br />
10 m/<br />
s<br />
εµ<br />
° °<br />
Useful Geometry<br />
Circle<br />
2<br />
Area = π r<br />
Circumference = 2π<br />
r<br />
Sphere<br />
Surface area = 4π<br />
r<br />
4 3<br />
Volume = π<br />
3<br />
r<br />
Cylinder<br />
Lateral surface<br />
area = 2π<br />
rL<br />
2<br />
Volume = π rL<br />
2