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Formula sheet with trigonometry and vectors, kinematics, quadratics, derivatives, integrals, constant, circular motion, forces and centre of mass.
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Trigonometry and Vectors:
sin 30
◦ = cos 60
1
2
sin 36. 9
◦ ≈ cos 53. 1
◦ ≈
3
5
sin 45
◦ = cos 45
1 √
2
sin 53. 1
◦ ≈ cos 36. 9
◦ ≈
4
5
sin 60
◦ = cos 30
√
3
2
hadj = h cos θ = h sin φ
hopp = h sin θ = h cos φ
h
2
= h
2
adj
2
opp
tan θ =
hopp
hadj
opp
Law of cosines: C
2 = A
2
2 − 2 AB cos γ
Law of sines:
sin α
sin β
sin γ
B γ
α
C
A
β
A = Ax
i + Ay
j + Az
k
~ A
|
~ A|
x
x
y
y
z
z
= AB cos θ = A ‖
‖
y
z
z
y
)ˆi + (A z
x
x
z
)ˆj + (A x
y
y
x
k
B| = AB sin θ = A⊥B = AB⊥ (direction via right-hand rule)
Quadratic:
ax
2
−b ±
b
2 − 4 ac
2 a
Derivatives: d
dt
(at
n ) = nat
n− 1
d
dt
sin at = a cos at
d
dt
cos at = −a sin at
Integrals:
t 2
t 1
f (t)dt =
a
n+
(t
n+
2
− t
n+
1
if f (t) = at
n , then
f (t)dt =
a
n+
t
n+
(n 6 = −1)
sin at dt =
− 1
a
cos at
cos at dt =
1
a
sin at
Kinematics:
translational rotational
〈~v〉 =
~r 2 −~r 1
t 2 −t 1
~v =
d~r
dt
〈~a〉 =
~v 2 −~v 1
t 2 −t 1
~a =
d~v
dt
d
2 ~r
dt
2
~r(t) = ~r 0
t
0
~v(t
′ ) dt
′
~v(t) = ~v 0 +
t
0
~a(t
′ ) dt
′
〈ω〉 =
θ 2 −θ 1
t 2 −t 1
ω =
dθ
dt
〈α〉 =
ω 2 −ω 1
t 2 −t 1
α =
dω
dt
d
2 θ
dt
2
θ(t) = θ 0
t
0
ω(t
′ ) dt
′
ω(t) = ω 0 +
t
0
α(t
′ ) dt
′
—– constant (linear/angular) acceleration only —–
~r(t) = ~r 0
t +
1
2
~at
2
~v(t) = ~v 0
v
2
x
= v
2
x, 0
(x − x 0
(and similarly for y and z)
~r(t) = ~r 0
1
2
(~v i
)t
θ(t) = θ 0
t +
1
2
αt
2
ω(t) = ω 0
ω
2
f
= ω
2
0
θ(t) = θ 0
1
2
(ω i
)t
Energy and Momenta:
translational rotational
1
2
M v
2
F · d~r
const
−−−→
force
F · ∆~r
dW
dt
F · ~v
p~ cm
= m 1
~v 1
~v 2
= M~v cm
F dt = ∆~p
Fext = M~acm =
d~p cm
dt
∑
~ F int
if
ext,x
= 0, p cm,x
= const
~τ = ~r ×
F and |~τ | = r⊥F = F⊥r
Krot =
1
2
Itotω
2
τ dθ
const
−−−→
torque
τ ∆θ
dW
dt
= ~τ · ~ω
~r × ~p
1
~ω 1
2
~ω 2
tot
~ω
~τext = Itot ~α =
d
dt
∑
~τint = 0
if
τext,z = 0, Lz = const
—– Work-energy and potential energy —–
tot,i
other
tot,f
U (r) = −
F · d~r ; Ugrav = M gycm ; Uelas =
1
2
k∆x
2
Fx(x) = −dU (x)/dx
∂U
∂x
i +
∂U
∂y
j +
∂U
∂z
k
Constants/Conversions:
g = 9. 80 m/s
2
= 32. 15 ft/s
2
(Earth, sea level)
≈ 10 m/s
2
≈ 33 ft/s
2
− 11 N · m
2 /kg
2 1 mi = 1609 m
1 lb = 4. 448 N 1 ft = 12 in
⇔ 0. 454 kg (Earth, sea level) 1 in = 2. 54 cm
1 rev = 360
◦ = 2π radians
Circular motion: arad =
v
2
atan =
d|~v|
dt
= Rα
2 πR
v
s = Rθ v tan
= Rω
Relative velocity: ~vA/C =^ ~vA/B +^ ~vB/C
~v A/B
= −~v B/A
Forces:
Newton’s Law:
F = m~a,
FB on A = −
FA on B
Hooke’s Law: F x
= −k∆x
friction: |
f s
| ≤ μ s
|~n|, |
f k
| = μ k
|~n|
Centre-of-mass:
~r cm
m 1
~r 1
~r 2
+... + m n
~r n
m 1
+... + m n
(and similarly for ~v and ~a)
Gravity:
grav
r
2
rˆ U grav
r
Kepler’s Laws:
st :
nd : ~r × ~v = constant
rd : T =
2 πa
3 / 2
Moments of inertia:
Thin cylinder
2
Thin cylinder
1
2
2
1
12
2
Hollow sphere
2
3
2
Solid sphere
2
5
2
Solid cylinder
1
2
2
Solid cylinder
1
4
2
1
12
2
Thin rod
1
12
2
Thin rod
1
3
2
Thick cylinder
1
2
2
1
2
2
Thick cylinder
1
4
2
1
2
2
1
12
2
Rectangular plate
1
12
M (a
2
2 )
Rectangular plate
1
3
M a
2
For a point-like particle of mass M a distance R from the axis of rotation: I = M R
2
Parallel axis theorem: Ip = Icm + M d
2
A disk is a cylinder of negligible length; the I for a disk may be found by setting L = 0 in the formulae for cylinders
Periodic motion:
ω = 2πf = 2π/T
pendulum : T = 2π
L/g = 2π
P
/mgd
spring : T = 2π
m/k
torsion : T = 2π
I/κ
Simple harmonic motion:
d
2 x
dt
2
2 x = 0
⇔ a(t) = −ω
2 x(t)
or α(t) = −ω
2 θ(t)
x(t) = A cos (ωt + φ 0
v(t) = −ωA sin (ωt + φ 0
a(t) = −ω
2
A cos (ωt + φ 0 )
tan φ 0
−v 0
ωx 0
2 = x
2
0
v 0
ω
2