Title | PHYS1001 Formula Sheet 2020 |
---|---|
Author | Mick Luu |
Course | Physics for Scientists and Engineers |
Institution | University of Western Australia |
Pages | 6 |
File Size | 138.4 KB |
File Type | |
Total Downloads | 35 |
Total Views | 134 |
formula sheet...
Semester 2 Examinations
Page 3 of 8
PHYS1001 data & formulae
The following equations and data might be useful: Acceleration due to gravity at earth’s surface:
g = 9.80 m s−2
Speed of light in a vacuum
c = 3.00 × 108 m s−1
Permittivity of free space Mass of one proton Mass of one electron Charge of an electron
ǫ0 = 8.85 × 10−12 F m−1 mp = 1.673 × 10−27 kg me = 9.11 × 10−31 kg e = 1.60 × 10−19 C
Boltzmann’s constant Planck’s constant
kB = 1.38 × 10−23 J K−1 h = 6.626 × 10−34 J s = 4.136 × 10−15 eV s ~=
h = 1.055 × 10−34 J s 2π = 6.582 × 10−16 eV s σ = 5.67 × 10−8 W m−2 K−4 R∞ = 13.606 eV R = 8.314 J K−1 mol−1
The Stefan-Boltzmann constant Rydberg The universal gas constant
cwater = 4184 J kg−1 K−1
Specific heat of liquid water
cice = 2050 J kg−1 K−1
Specific heat of ice Heat of fusion for water
Lf,water = 3.34 × 105 J kg−1
Heat of vapourisation for water Speed of sound in air
Lv,water = 2.26 × 106 J kg−1 = 343 m s−2
Density of water (20◦ C and 1 atm) Conversion factors:
= 1.00 × 103 kg m−3 1 eV = 1.60 × 10−19 J
Area of a Sphere:
0 ◦ C = 273.15 K 1 L = 10−3 m3 A = 4πr 2
Prefixes: f = 10−15 , p = 10−12, n = 10−9 , µ = 10−6 , m = 10−3 , k = 103 , M = 106 , G = 109 , T = 1012
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Page 4 of 8
Semester 2 Examinations
PHYS1001 data & formulae
Heat & Thermodynamics equations Thermal expansion:
∆L = αLi ∆T
Heating/Cooling:
Q = mc∆T
Thermal motion in a gas:
Kave,trans = 21 mv 2th = 32 kT
Heat Transfer by radiation:
4 Pnet = Pabs − Pem = eσA(T env − T 4)
Heat Transfer by conduction:
H=
First Law and Work:
∆U = Q + W
Ideal Gas Law:
pV = nRT
Internal energy (ideal gas):
U = 32 nRT (monatomic)
γ (ideal gas):
γ=
∆V = β Vi ∆T Q = mL
c = kA Th −T L
Q t
β = 3α
vth =
p
3kT /m
H is heat flow in watts. RV W = − V f p dV i
Where n is the number of moles of gas. ∆U = nCV ∆T
Cp CV
γmonatomic = γdiatomic =
5 3
7 5
γpolyatomic =
4 3
Vf Vi
Wadiabatic =
Work (ideal gas):
Wisothermal = −nRT ln
Specific Heat (ideal gas):
Q = nCV ∆T
Q = nCp ∆T
Cp = CV + R
CV = f2 R
Adiabatic process in ideal gas:
pV γ = constant
Entropy change:
∆S =
Q T
T V γ−1 = constant R f dQ (constant T ) ∆S = i T
pf Vf −pi Vi γ−1
∆S = mc ln
Mechanics equations
p = mv v=ω×r
dp dt τ =r×F F=
L = Iω
τ=
L=r×p
Iz =
dL dt X
mi ri2
i
1 Ktrans = mv 2 2 dU F (x) = − dx
Krot
1 = Iω 2 2
f ≤ µs N
f = µk N
GMm Ugrav = − + U0 r Z x F (x)dx = U (x0 ) − U (x) x0
dr Circular motion: v = = r ϑ˙ eˆϑ dt Kinematics:
Fgrav
GMm =− 2 r
v = v0 + at
dv a= = −rϑ˙2 ˆer = −ω 2 r dt 1 x = x0 + v0 t + at2 v 2 = v 20 + 2a(x − x0 ) 2
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Tf Ti
Semester 2 Examinations
Page 5 of 8
PHYS1001 data & formulae
Waves & Optics equations 1 T
Frequency:
f=
Angular Frequency:
ω = 2πf
Wave number:
k=
Average Power of Wave on a String:
P¯
Intensity:
I=
Standing Waves:
L=
Doppler Effect:
2π λ = 21 µvω 2 A2 P A
n 2 λ, L=m 4 λ, f ′ = 1±f u v
n = 1, 2, 3, ... m = 1, 3, 5, ....
Snell’s Law:
n1 sin θ1 = n2 sin θ2
Refractive Index:
n=
Critical Angle:
sin θc =
Double Slit (Bright Fringes)
d sin θ = mλ,
Double Slit (Dark Fringes)
d sin θ = (m +
N Slit (Bright Fringes)
d sin θ = mλ,
N Slit (Dark Fringes)
d sin θ =
Single Narrow Slit (Destructive):
a sin θ = mλ,
Rayleigh Criterion (single slit):
θmin =
Law of Malus:
I = I0 cos2 θ
Trigonometric Identities:
sin( π2 ± x) = cos x
c v n2 n1
m N λ,
m = 0, 1, 2, ... 1 2 )λ,
m = 0, 1, 2, ...
m = 0, 1, 2, ... m = 1, 2, 3, ... AN D m 6= multiple of N m = 1, 2, 3, ...
λ a
sin α ± sin β = 2 sin 12 (α ± β) cos 21(α ∓ β) cos α + cos β = 2 cos 12 (α + β) cos 12 (α − β) cos α − cos β = 2 sin 12 (α + β) sin 12 (β − α)
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Page 6 of 8
Semester 2 Examinations
PHYS1001 data & formulae
Electricity equations Vsphere = 43 πr 3
Asphere = 4πr2
Acircle = πr 2
Ccircle = 2πr
Electric Force:
~ = qE ~ F
Electrical Potential:
V =
Potential difference:
∆V = −
Field of point charge:
~ = E
Potential of point charge:
V =
Gauss’s Law:
ΦE =
Electric Field from Potential:
~E = −∇V ~ = −( ∂V , ∂V , ∂V ) ∂x ∂y ∂z
Field of Sphere:
~E =
U q
Rb
~ · d~l E
a 1 q ˆ 4πǫ0 r2 r 1 q 4πǫ0 r
~ · dA ~ = E
H
Field near conducting sheet:
1 q 4πǫ0 r2 Esheet = σǫ0
Field near non-conducting sheet:
Esheet =
Field of linear charge distribution:
Eline =
Capacitance:
C=
Parallel plate Capacitor:
Ck =
qenclosed ǫ0
rˆ
σ 2ǫ0
λ 2πǫ0 r
Q V ǫ0 A d
∆V = Ed UC = 12 CV 2
Capacitor Energy:
Breakdown of Classical Physics equations E c = fλ, f= , h p 2 2 E = |~ p | c + m2 c 4 ,
E = |~ p|c
λ=
h p
I(T ) = σT 4 λmax T = 2.898 × 10−3 m K λ sin θ = m , m = 1, 2, 3, . . . a h L = n~ = n , n = 1, 2, 3, . . . 2π ~ ~ ∆p ∆x ≥ , ∆E ∆t ≥ 2 2 2 RZ E = − 2 , where R = 13.606 eV n
for photons
Kmax = hf − Φ, h (1 − cos φ) mc p 2m(U − E) −2bL T ≈e , where b = ~ n2 ǫ0 h2 rn = , me vr = n~ Zπe2 me
∆λ = λ′ − λ =
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Semester 2 Examinations
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PHYS1001 data & formulae
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Semester 2 Examinations
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PHYS1001 data & formulae
THIS PAGE HAS BEEN INTENTIONALLY LEFT BLANK. It may be used for rough working which will NOT be marked.
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