physics 2a: additional equations for the final celebration
TRANSCRIPT
Physics 2A: Additional Equations for the Final Celebration
Chapter 10: Energy and Work ⇒ the total energy of a system is the sum of all of the different kinds of energy in the system: E = K + Ug + Us + Eth + Echem + … ⇒ energy within a system can be transformed from one form of energy into another; energy can be transferred to or from a system by doing work on it Work: cosW Fd θ=
⇒ The unit of work is the Joule (J). 1 J = 1 Nm = 1 kg m2/s2
⇒ Work can be +, -, or 0. Work Energy Theorem: The total energy of a system changes by the amount of work done on it:
...g s th chemE K U U E E W∆ = ∆ + ∆ + ∆ + ∆ + ∆ + = Law of conservation of energy: The total energy of an isolated system (no work is done on the system) remains constant:
... 0g s th chemE K U U E E∆ = ∆ + ∆ + ∆ + ∆ + ∆ + =
Kinetic Energy: 212K mv=
Gravitational Potential Energy: gU mgy=
Elastic Potential Energy: 212sU kx=
Thermal energy: th kE f x∆ = ∆ Conservation of Mechanical Energy: The mechanical energy of an isolated system without friction is conserved:
( ) ( ) ( ) ( )f g f s f i g i s iK U U K U U+ + = + + ⇒ If there is friction, the total energy is conserved:
( ) ( ) ( ) ( )f g f s f th i g i s iK U U E K U U+ + + ∆ = + +
Power: The rate at which energy is transformed or work is done: EP t
WP t
∆= ∆
= ∆
Chapter 11: Using Energy
∆E = ∆K + ∆Ug + ∆Us + ∆Eth + ∆Echem + … = W ⇒ energy is never created or destroyed, only transferred into different forms ⇒ when we say that energy is “lost”, is isn’t actually lost but converted into a non-useful form, usually thermal energy
Efficiency: what you getwhat you had to payfor
out
in
EeE
= =
⇒ the efficiency of the human body is ~25% 1 Cal = 1000 cal = 4186 J
EP t∆= ∆ ⇒ the human body uses energy at a rate of ~100W when at rest
Temperature: ⇒ thermal energy Eth for an ideal gas equals the total energy of all moving atoms and molecules in the gas ⇒ the temperature of an ideal gas depends upon the average KE of the atoms and molecules in the gas
ice point steam point Celsius scale 0°C 100°C Kelvin scale 273K 373K Fahrenheit scale 32°F 212°F
273.15K CT T= +
⇒ for an ideal gas:
Kavg = 3/2 kBT Boltzmann’s constant: kB = 1.38 × 10-23 J/K
Eth = N Kavg = 3/2 NkBT
Chapter 12: Thermal Properties of Matter Atomic Model of Matter: ⇒ a special notation is used to indicate the composition of a nucleus: A
Z X Atomic number Z: # of protons in nucleus Atomic mass number A: # of protons + # of neutrons (N) A = Z + N X: chemical symbol for element Atomic mass unit: 1 u = 1.6605 × 10-27 kg n → # of moles N → # of particles NA → 6.022 × 1023 mol-1
(in grams)
mol
MnM
= where Mmol is the molar mass
⇒ the mass per mole (g/mol) of a substance has the same numerical value as the
atomic or molecular mass of the substance (in u) Ideal Gas Law: pressure: p = F/A unit of p is the Pascal (Pa); 1 Pa = 1 N/m2
8.31 JPV nRT R mol K= =
221.38 10 JPV NkT k K
−= = ×
⇒ if the number of moles is constant: f f i i
f i
p V pVT T
=
Heat: heat (Q): energy transferred between objects because of a temperature difference
Q > 0 if object absorbs heat Q < 0 if object loses heat
Q Mc T= ∆ where c = specific heat capacity
cwater=4186 J/kg•K
⇒ during a phase change, heat is absorbed or lost but the temperature doesn’t change solid to liquid / liquid to solid Q = +MLf (Lf = latent heat of fusion) liquid to gas / gas to liquid Q = +MLv (Lv = latent heat of vaporization)
for water: Lf = 3.33 × 105 J/kg Lv = 22.6 × 105 J/kg ⇒ for two objects that are placed in thermal contact (assuming no heat is lost to the surroundings): Qnet = Q1 + Q2 = 0 Heat Transfer: ⇒ heat is transferred by three processes: convection, conduction, and radiation
conduction: Q kAP Tt L
= = ∆ ∆
k = thermal conductivity (units are W/m•K)
radiation: 4QP e T At
σ= =∆
(radiation emitted)
40
QP e T At
σ= =∆
(radiation absorbed)
Stefan-Boltzmann’s constant 8
2 45.67 10 Wm Kσ −= ×
net power radiated: Pnet = Pemitted - Pabsorbed
Chapter 13: Fluids Density: m
Vρ = 331.000 10water
kgmρ = ×
Pressure:
Pressure: FpA
= patm=1.013 × 105 Pa = 1 atm
Pressure in a Fluid: 0p p gdρ= + Buoyancy: Archimede’s Principle: the magnitude of the buoyant force on an object partially or completely immersed in a fluid equals the weight of the fluid displaced Buoyant Force: B fluid subF V gρ= ⇒ if an object is completely submerged, Vsub = Vobj
⇒ if an object is floating, FB = w = mg Fluids in Motion: Equation of Continuity: 1 1 1 2 2 2A v A vρ ρ= ⇒ if the fluid is incompressible (ρ1=ρ2): 1 1 2 2A v A v=
⇒ the volume flow rate Q = Av Bernoulli’s Equation: 2 2
1 1 1 2 2 21 1
2 2p v gy p v gyρ ρ ρ ρ+ + = + +
Bernoulli’s Principle: where the speed of a fluid increases, the pressure in the fluid decreases
Chapter 14: Oscillations Frequency: 1f T= (units of f = Hz)
Period: 1T f= (units of T = s)
Hooke’s law: F kx= − (units of k = N/m) ⇒ the – sign indicates that the direction of the force is opposite the displacement Simple Harmonic Motion: ⇒ for an object oscillating in simple harmonic motion:
max
max2 2
max
cos(2 )(2 )sin(2 ) (2 )
(2 ) cos(2 ) (2 )
x A ft x Av A ft ft v A ft
a A ft ft a A ft
ππ π π
π π π
= == − =
= − =
Note: v = 0 at x = +A; v = vmax at x = 0 a = 0 when x = 0; a=amax at x = +A
Energy in SHM: 2 2
2 2max
1 12 2
1 12 2
E mv kx
E mv kA
= +
= =
⇒ for a mass m oscillating on a spring with spring constant k:
1 22
k mf Tm k
ππ
= =
Pendulums:
⇒ for a simple pendulum (for small angles):
1 22
g Lf TL g
ππ
= =
Chapter 15: Traveling Waves and Sound Waves: Transverse Wave: the disturbance occurs perpendicular to the direction of travel of the wave Longitudinal Wave: the disturbance occurs parallel to the direction of travel of the wave
1 1f TT f
= = v v fTλ λ= =
⇒ if the frequency is increased, the wavelength is decreased but wave speed doesn’t change
Speed of waves on a string: sT mvL
µµ
= =
Doppler Effect: 0
0
1
1s
s
vvf f vv
± =
Chapter 16: Superposition and Traveling Waves Linear Superposition: The Principle of Linear Superposition: when two or more waves are present at the same place at the same time, the resultant disturbance is the sum of the disturbances from the individual waves ⇒ for 2 wave sources vibrating in phase:
0,1,2,... constructive interference
1( ) 0,1,2,... destructive interference2
r m m
r m m
λ
λ
∆ = =
∆ = + =
Beats: 1 2beatsf f f= − Standing Waves: ⇒ for standing waves on a string fixed at both ends:
2 1,2,3,...2m m
L vf m mm L
λ = = =