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Formula sheet in given trigonometry and vectors, quadratics, derivatives, integrals, kinematics, circular motion, relative velocity, forces, energy and momentums.
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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 + m 2 ~v 2 +...
= M~vcm
F dt = ∆~p
ext
= M~a cm
d~pcm
dt
∑
~ Fint = 0
if
Fext,x = 0, pcm,x = const
~τ = ~r ×
F and |~τ | = F⊥r = F l
Krot =
1
2
Itotω
2
τ dθ
const
−−−−→
torque
τ ∆θ
dW
dt
= ~τ · ~ω
~r × ~p
= I 1 ~ω 1 + I 2 ~ω 2 +...
= Itot~ω
~τext = Itot ~α =
d
dt
∑
~τ int
if
τ ext,z
z
= const
—– Work-energy and potential energy —–
tot,i
other
tot,f
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 vtan = Rω
Relative velocity: ~vA/C =^ ~vA/B +^ ~vB/C
~vA/B = −~vB/A
Forces:
Newton’s:
F = m~a,
FB on A = −
FA on B
Hooke’s: Fx = −k∆x
friction: |
fs| ≤ μs|~n|, |
fk| = μk|~n|
Centre-of-mass:
~r cm
m 1
~r 1
~r 2
+... + m n
~r n
m 1 + m 2 +... + mn
(and similarly for ~v and ~a)
Moments of inertia:
rectangular plate,
axis through centre
thin rectangular plate,
axis along edge
hollow sphere
solid sphere
thin-walled hollow
cylinder
solid cylinder
1
12
2 I =
1
3
2 I =
1
12
M (a
2
2 ) (^) I =
1
3
M a
2
a
through centre
slender rod, axis
through one end
slender rod, axis
thin-walled
2
hollow cylinder
b
a
b L
1
2
2
1
2
2
1
2
2 I = M R
2
2
5
2 I =
2
3
2
For a point-like particle of mass M a distance R from the axis of rotation: I = M R
2
Parallel axis theorem: I p
cm
2