equations of physics
DESCRIPTION
List of Physics EquationsTRANSCRIPT
-
Copyright 2007 The Open University WEB 96146 9
S207
STANDARD EQUATIONS AND
CONSTANTS
This complete list of constants, mathematical formulae and physics
equations is included for reference. It may be useful as an aid to your
memory but please bear in mind that many of the entries will not be
needed in this examination.
-
2Useful constants
magnitude of the acceleration
due to gravity on Earth g = 9.81 m s2
Newtons universal
gravitational constant G = 6.673 1011 N m2 kg2
Avogadros constant Nm = 6.022 1023 mol1
Boltzmanns constant k = 1.381 1023 J K1
molar gas constant R = 8.314 J K1 mol1
permittivity of free space 0 = 8.854 1012 C2 N1 m2
1/40 = 8.988 109 N m2 C2
permeability of free space 0 = 4 107 T m A1
speed of light in vacuum c = 2.998 108 m s1
Plancks constant h = 6.626 1034 J s
" = h/2 = 1.055 1034 J s
Rydberg constant R = 1.097 107 m1
Bohr radius a0 = 5.292 1011 m
atomic mass unit amu (or u) = 1.6605 1027 kg
charge of proton e = 1.602 1019 C
charge of electron e = 1.602 1019 C
electron rest mass me = 9.109 1031 kg
charge to mass ratio of
the electron e/me = 1.759 1011 C kg1
proton rest mass mp = 1.673 1027 kg
neutron rest mass mn = 1.675 1027 kg
radius of the Earth 6.378 106 m
mass of the Earth 5.977 1024 kg
mass of the Moon 7.35 1022 kg
mass of the Sun 1.99 1030 kg
average radius of Earth orbit 1.50 1011 m
average radius of Moon orbit 3.84 108 m
-
3Mathematical formulae
2 4
2
b b acx
a
=
2 rad = 360
sin( 2 ) sin( ) + =
cos( 2 ) cos( ) + =
sin( ) sin( ) =
cos( ) cos( ) =
2 2sin ( ) cos ( ) 1 + =
sin( )tan( )
cos( )
=
a b = ab cos
a b = axbx + ayby + azbz
a b = (aybz azby, azbx axbz, axby aybx)
|a b | = ab sin
If d
dt=
v
v , then v(t) = v0 e t
ex ey = ex+y
(ex)y = exy
ex = 1/ex
logeex = x
1
N
i i
i
x p x
=
=
sphere surface area = 4r2
sphere volume = 34
3
r
Derivatives
[A, n, k and are constants; x, y and z are
functions of t]
xd
d
x
t
A 0
tn ntn1
sin( t) cos( t)
cos( t) sin( t)
ekt kekt
Ayd
d
yA
t
y + zd d
d d
y z
t t+
-
4Book 2 Describing motion
x xs t= v ( constant)
x=v
1 2
2x x xs u t a t= +
x x xu a t= +v
2 2 2x x x x
u a s= +v
1
2( )
x x xs u t= +v
t= +u av
1 2
2t t= +s u a
arcs R =
d 2 rad
dt T
= =
2 rr
T
= =v
2
2a rr
= = =v
v
22 f
T
= =
( ) sin( )x t A t = +
2
2
2
d ( )( )
d
x tx t
t
=
2 2
2 21
x y
a b+ =
2 21
e a ba
=
2
3
TK
a=
-
5Book 3 Predicting motion
F = ma
W = mg
1 2
212
Gm m
r
=F r
Fmax = staticN
F = slideN
F = 6Rv
2
2m
F mrr
= =
v
Fx = ksx
s
22
mT
k
= =
22
lT
g
= =
1 2trans 2E m= v
W = F s
Egrav = mgh
1 2str s2
E k x=
1 2grav
Gm mE
r
=
potd
dx
EF
x
=
P = d
d
W
t = F v
x(t) = (A0 et /) sin( t + )
2 total stored energy
average energy loss per oscillationQ
=
0
2 2 20
/
( ) ( / )
F mA
b m 2=
+
p = mv
d
dt=
pF
= r F
v = r
d
dt=
2i i
i
I m r=
1 2rot 2
E I=
1 12 2kin CMCM2 2
E M I = +v
W =
P =
l = r p
L = I
=d
dt
L
-
6Book 4 Classical physics of matter
(number density)M
mV
= =
FP
A
=
3m r m10 kgM M N m
= =
1 d
d
V
V T =
1 d
d
V
V P =
PV nRT NkT= =
2 2
f fU nRT NkT= =
3trans 2
E kT =
p = A eE /kT
2 2( ) exp( /2 )f B m kT= v v v
3 / 2
42
mB
kT
=
mp
2kT
m=v
8kT
m =
v
rms
3kT
m=v
/( ) e E kTg E C E =
3 / 22 1
CkT
=
1mp 2
E kT=
32
E kT =
tot
2
fE kT =
W = PV
U = Q + W
QC
T=
2V
fC nR=
P VC C nR= +
21
P
V
C
C f = = +
PV = I
PV A =
revQ
ST
=
2 2
2 1 e e
1 1
log logV PP V
S S C CP V
= +
S = k logeW
c
h h
1W T
Q T = =
c c
h c
Q T
W T T = =
AP P g z= +
( ) (0)exp( / )P z P z =
kT
mg =
2 1
1 2
A
A=
v
v
1 2
2constantP gh + + =v
F Ax
=
v
0 0LRe
=
v
-
7Book 5 Static fields and potentials
1 2grav 2
Gm m
r= F r
1 2
el 20
1
4
q q
r=
F r
Fgrav (on m at r) = mg(r)
Fel (on q at r) = qe(r)
20
( )4
Q
r
=
r re
1 2grav
Gm mE
r=
1 2
el
04
q qE
r=
Eel (with q at r) = qV(r)
0
1( )
4
QV
r
=
r
d ( )
dx
V
x=
r
E
qC
V=
C = r 0A
d
2 2
el2 2 2
qV CV qE
C= = =
d
d
qi
t=
i neA= v
R| |
| |
VR
i=
LR
A
=
V iR=
eff i
i
R R=
=i iRR
11
eff
2
2V
P iV i RR
= = =
EMFV V ir=
/0 e
tq q =
/0 e
ti i =
= RC
Fm = q [v B(r)]
0( )2
iB r
r
=
0
centre2
NiB
R
=
NiB
l
0=
F = q[e(r) + v B(r)]
C
1
2
q Bf
m
| |=
perpC
mR
q B
| |=
| |
v
H
iV B
nqt=
Fm = l[i B(r)]
mF Bil=
0 1 2
2
F i i
l d
=
iAB =
-
8Book 6 Dynamic fields and waves
cosAB =
ind
d ( )( )
d
tV t
t
| | =
ind
d ( )( )
d
i tV t L
t| | =
2ANL
l
=
1 2mag 2
E Li=
bat
d ( )( )
d
i tV L i t R
t =
( )bat /( ) 1 e Rt LV
i tR
=
Vmax
= imaxL
max
max
iV
C=
1
LC =
1
2
d ( )( )
d
i tV t M
t| | =
1 2N N AM
l
=
2
2 1
1
( ) ( )N
V t V tN
| | = | |
sin( )y A kx t=
2k
=
2
T
=
fk
= =v
TF
=v
obs emf fV
=
v
v
obs em
Vf f
=
v
v
( , ) 2 cos( )sin( )y x t A t kx=
2L n
=
c f =
1 2
2 1
sin
sin
i n
r n= =
v
v
1 2
crit
2 1
sinn
in
= =
v
v
sinn
n d =
sinw
=
1 1 1
u f+ =
v
m
u
=
v
P = 1/f
Ptotal = P1 + P2 + P3 +
IM
OB
M
=
o
e
fM
f=
light-gathering power =
2
o
p
D
D
maximum light-gathering power
=
22
o o
e e
D f
D f
=
exposure = It
-number f
FD
=
(Continued overleaf)
-
90
2 21 /
TT
V c
=
02
21
LL
V
c
=
( )x x Vt =
2( / )t t Vx c =
2
2
1
1V
c
=
21
x
x
x
V
V
c
=
v
v
v
2 21
m
c
=
p
v
v
2 2
d d
d d 1
m
t t c
= =
pF
v
v
2
tot2 21
mcE
c
=
v
Emass = mc2
2
2trans
2 21
mcE mc
c
=
v
2 2 2 2 4totE p c m c= +
E = cp
-
10
Book 7 Quantum physics: an introduction
E = hf
1 2e max2
m hf = v
mevr = n"
1
2n
EE
n
| |=
dB
h
p =
2x
x p "
2E t
"
( )2
tot pot2 2
d 2( ) 0
d
mE E x
x
+ =
"
2 2
kin2
kE
m=
"
p = "k
2 2
tot28
n hE
mD=
2
2 2 2tot 1 2 32
( )8
hE n n n
mD= + +
P = | (x1) |2x
P = |1(r) |2V = |1(r) |2 4r2r
4e
tot2 2 2 2
0
1 13.6eV
8
m eE
n h n
= =
( 1)L l l= + "
Lz = ml"
( 1)S s s= + "
Sz = ms"
-
11
Book 8 Quantum physics of matter
3/ 2
/2 1( ) e E kTN
G E EkT
=
( )D E B E=
3
3 2
3
2(2 )
LB m
h
=
B ( )
1( )
e 1E kTF E
=
B
1( )
e 1E kTF E =
FF ( )
1( )
e 1E E kTF E
=
+
Dp(E) = CE2
2p /
1( )
e 1E kTG E CE=
C = 8V/h3c3
N = 2.4C(kT)3
4
4( )15
U C kT
=
3
UP
V=
m
m
zNn
V=
e( )D E B E=
3 2e
3
4(2 )
VB m
h
=
Fe ( ) /
1( )
e 1E E kTG E B E
= +
2 32
F
e
3
8
h nE
m
=
3F5
U NE=
2F5
P nE=
d
d
NN
t=
N(t) = N0 exp(t)
[END OF BOOKLET]