NEWTON’S LAWS 1. First Law: An object remains in its state of rest or motion with constant velocity unless acted upon by a net external force. dp F = 2. Second Law: Fnet = ma dt 3. Third Law: For every action there is an equal and opposite reaction. Weight
Fw = mg
Normal force
FN = mg cos θ (θ is the angle to the horizontal)
h
h
F p
1
V
p
q
Kinetic friction fk = µk FN
µs is the coefficient of static friction. µk is the coefficient of kinetic friction. For a pair of materials, µk < µs .
W = F · s = F s cos θ � W = F · ds
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mv 2 Centripetal force Fc = r
ˆ a = axˆi + ayˆi + az k
Magnitude
a = |a| =
Dot product
a · b = ax bx + ay by + az yz = ab cos θ
�
a2x + a2y + a2z
Cross product
a × b = (ay bz � � ax � = �� ax � ˆi
axb
Gravitational potential energy
Ug = mgh
Total mechanical energy
E = KE + U
Average power
Pavg =
Instantaneous power
MOMENTUM AND IMPULSE Linear momentum
p = mv
Impulse
J = �Ft = ∆p J= F dt = ∆p
a
COLLISIONS b
ˆ − az by ) ˆi + (az bx − ax bz) ˆj + (ax by − ay bx ) k � ay az �� ay bz �� ˆj ˆ � k
UNIFORM CIRCULAR MOTION v2 Centripetal acceleration ac = r
q
2
FRICTION Static friction fs, max = µs FN
h
V
p
q
5
KINEMATICS Average velocity
vavg =
∆s ∆t
DISTANCE s (m)
Instantaneous ds v= velocity dt
Displacement ∆s =
Average acceleration
�
aavg =
v dt
∆v ∆t
Instantaneous dv a= acceleration dt
Change in velocity
vf = v0 + at 1 vavg = (v0 + vf ) 2
s = s0 + v0 t +
1 at 2
= s0 − vf t +
1 at 2
= s0 + vavg t
=
v02
VELOCITY v (m/s)
+
t (s)
∆v =
�
CONSTANT ACCELERATION
vf2
t (s)
a dt
– ACCELERATION a (m/s2)
+
t (s)
–
+ 2a(sf − s0 ) CONTINUED ON OTHER SIDE
SPARKCHARTS™ Physics Formulas page 1 of 2
PhysicsForm 8.0 4/15/03 12:16 PM Page 2
WAVES
ELECTRICITY
T
WAVE ON STRING Tension in string FT
Mass density µ =
Length L
mass length
F =k
Electric field
E=
Potential difference
W ∆V = q
Fon q q
F = Eq
CIRCUITS ∆Q ∆t
Current
I=
Resistance
R=ρ
Ohm’s Law
I=
SOUND WAVES
Power dissipated by resistor
P = V I = I 2R
Beat frequency
Heat energy dissipated by resistor
W = P t = I 2 Rt
Speed of standing wave
v=
Wavelength of standing wave
λn =
FT µ
2L n
fbeat = |f1 − f2 |
DOPPLER EFFECT Motion of source Stationary
Motion of observer
Stationary
v λ
f
veff = v + vo λeff = λ � � o feff = f v+v v
Towards source at vo
Toward observer at vs
Away from observer at vs
veff = v � � s λeff = λ v−v � v � v feff = f v−v s
veff = v � � s λeff = λ v+v � v � v feff = f v+v s
veff = v ± vo � � s λeff = λ v±v v � � o feff = f v±v v±vs
Away from source at vo veff = v − vo
λeff = λ � � o feff = f v−v v
ROTATIONAL MOTION Angular position
Angular velocity
ωavg =
∆θ ∆t
ω=
v r dθ dt at r dω dt
ω=
α=
Angular acceleration
αavg =
s r
∆ω ∆t
α=
a
CONSTANT ωf = ω0 + αt
T = 2π
�
v=0 U = max KE = 0
MASS-SPRING SYSTEM
R
R
sphere
R
MR 2 ring
disk
Elastic potential energy
Period 2 MR 2 5
L
rod
TORQUE AND ANGULAR MOMENTUM Torque
τ =
dL dt
F = −k(∆)x ∆x is the distance the spring is stretched or compressed from the equilibrium position, and k is the spring constant.
1 ML2 12
R
R2 R3
Magnetic force on moving charge
F = qvB sin θ
F = q (v × B)
Magnetic force on current-carrying wire
F = BI� sin θ
F = I (� × B)
MAGNETIC FIELD PRODUCED BY… Magnetic field due to a moving charge
B=
µ0 qv × ˆr 4π r2
Magnetic field produced by a current-carrying wire
B=
µ0 I 2π r
Magnetic field produced by a solenoid
B = µ0 nI
Biort-Savart Law
dB =
Lenz’s Law and Faraday’s Law
ε=−
MAXWELL’S EQUATIONS � Gauss’s Law
�s
Gauss’s Law for magnetic fields
�s
Restoring force
MOMENTS OF INERTIA (I ) � I= r 2 dm Moment of inertia 1 MR 2 2
mg cos 0
v=0 U = max KE = 0
equilibrium position
= θ0 + ωavg t
MR 2
v = max U = min KE = max
τ = F r sin θ τ =r×F τ = Iα
Angular momentum
L = pr sin θ
L=r×p
L = Iω
Rotational KE rot = 12 Iω 2 kinetic energy
GAS LAWS Universal Gas Law
P V = nRT
Combined Gas Law
P2 V2 P1 V1 = T2 T1
2π T
=
�
1 k(∆x)2 2 � m T = 2π k Ue =
x = A sin(ωt)
Equation of motion
where ω =
k m
is the angular frequency
and A = (∆x)max is the amplitude.
THERMODYNAMICS 1. First Law ∆ (Internal Energy) = ∆Q + ∆W 2. Second Law: All systems tend spontaneously toward maximum entropy. ∆Qout Alternatively, the efficiency e = 1 − ∆Qin of any heat engine always satisfies 0 ≤ e < 1. Boyle’s Law
Loop rule: The sum of all the (signed) potential differences around any closed loop is zero. Node rule: The total current entering a juncture must equal the total current leaving the juncture.
PENDULUM
v=
V R
KIRCHHOFF’S RULES
SIMPLE HARMONIC MOTION
θ=
L A
Faraday’s Law
c
�
Ampere’s Law
�c
Ampere-Maxwell Law
c
E · dA =
r) µ0 I (d� × ˆ r2 4π
dΦB dt
Qenclosed ε0
B · dA = 0 E · ds = −
4
�
SPARKCHARTS
�� t
1 q1 q2 q1 q2 = 4πε0 r 2 r2
Coulomb’s Law
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Wave speed v = f λ Wave equation � � y(x, t) = A sin(kx − ωt) = A sin 2π λx −
ELECTROSTATICS
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2π T
∂ ∂ΦB =− ∂t ∂t
�
s
B · dA
B · ds = µ0 Ienclosed B · ds = µ0 Ienclosed + µ0 ε0
∂ ∂t
�
s
E · dA
GRAVITY m1 m2 r2
Newton’s Law of Universal Gravitation
F =G
Acceleration due to gravity
a=
Gravitational potential
U (r) = −
Escape velocity
vescap e
20593 36340
ω = 2πf =
7
1 2π = f ω
Angular frequency ω
TM
Period T
Contributors: Bernell K. Downer, Anna Medvedovsky Design: Dan O. Williams Illustration: Dan O. Williams, Matt Daniels Series Editors: Sarah Friedberg, Justin Kestler
T =
Wavelength λ
Report errors at www.sparknotes.com/errors
Frequency f
Amplitude A
GM Earth 2 rEarth
GM m r � GM = r
KEPLER’S LAWS OF PLANETARY MOTION 1. Planets revolve around the Sun in an elliptical path with the Sun at one focus. 2. The imaginary segment connecting the planet to the Sun sweeps out equal areas in equal time. 3. The square of the period of revolution is directly proportional to the cube of the length of the semimajor axis of revolution: T 2 is constant. a3
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