AP Physics B Review

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AP Physics B Review --- ASHWIN JACOB
Exam 1
Kinematics
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Definition: The Description of Motion
Projectile- an object that’s influenced by gravity and in motion
o Horizontal and vertical components are independent
o The horizontal component of the velocity remain constant
o The vertical component has a constant acceleration of “g” or 9.8 m/s2
o Only the vertical component of velocity, at its maximum height, is equal to zero
Kinematic Formulas
1) 𝑣̅ =
2) 𝑣̅ =
3) 𝛼 =
βˆ†π‘‘
βˆ†π‘‘
𝑉𝑓 +𝑣𝑖
2
Δv
Δt
=
𝑉𝑓 −𝑣𝑖
𝑑
4) π‘₯𝑓 = π‘₯𝑖 + 𝑣𝑖 𝑑 + 1⁄2 π‘Žπ‘‘ 2
5) 𝑣𝑓 2 = 𝑣𝑖 2 + 2π‘ŽΔπ‘₯
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Acceleration(α) is the rate that velocity change
o Occurs when there is a change of speed or change of motion
When doing projectile problems, it is your choice on what direction is positive and what direction is
negative
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Shortcut for velocity of free-falling object 𝑣 = √2π‘”βˆ†π‘¦
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Analyzing Graphs
o Area of Graph is the distance
o Graph B
 From A(1st point) to x-axis, it has a negative velocity(backward) and since below x-axis it
is negative distance
Line 2
velocity
Line 1
6
12
10
8
6
4
2
0
4
2
0
-2
0.00
5.00
15.00
Time
25.00
-4
-6
Series 1
0
5
10
15
Exam 2
Vectors ****Degree Mode****
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Vectors- Quantities that require both size(magnitude) and direction
o Velocity, Displacement, and Force
Scalars-Magnitude Only
o Volume, Mass, Distance, Speed
Vector Equations
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o π‘₯ = 𝑅 × cos πœƒ
o 𝑦 = 𝑅 × sin πœƒ
o ∑ π‘₯ = 𝐴π‘₯ − 𝐡π‘₯
βƒ— = √∑ π‘₯ 2 + ∑ 𝑦 2
o 𝑅
o πœƒ = tan−1 (
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∑𝑦
∑π‘₯
)
Vector Example
o → =50m @ 40o N of E
A
o → = 20π‘š @ 30π‘œ 𝑁 π‘œπ‘“ π‘Š
𝐡
N
A
B
B
30o
40o
y
W
B
A
x
x
Plug in the values into
the 1st and 2nd equations
to get the x and y values of
A A and B. From there, you
y Can solve for anything you
Want
E
S
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Vector Rules
o If the two X’s or Y’s are going in the same direction, then add the x-vectors or y-vectors vector
o If the two X’s or Y’s are going in the opposite direction, subtract the bigger x-value or y-value
from the smaller x-value or y-value(the direction it will be heading is the big value’s direction)
o Subtracting Vectors
βƒ— = 𝐴 + (−𝐡
βƒ—)
 𝐴−𝐡
 Just the opposite of B = Same Angle, Same Meter, Different Direction
Two-Dimension Kinematics
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The horizontal and vertical motions of a projectile are independent of one another
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Changed Equations
o 𝑦𝑓 = 𝑦𝑖 + 𝑣𝑖 𝑑 + 1⁄2 π‘Žπ‘‘ 2
o π‘₯ = 𝑣̅ 𝑑
o Still Need to consider the angles
Newton’s First Law (Law of Inertia)
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Inertia- tendency of an object to resist change in their motion
o Depends on the amount of mass(kg)
Newton’s First Law
o An object at rest will remain at rest
o An object in motion will remain in motion in a straight line at a constant speed unless acted
upon a Net External Force(push or pull)
Newton’s Second Law
o 𝐹𝑛𝑒𝑑 = π‘šπ‘Ž
o Two things to Remember
 Vector Equation
 Net Force and Acceleration MUST have the same direction!!!
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FN
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o 𝐹 = π‘šπ‘” (Definition of Weight)
Force is measured in kg*m/s2 or Newton
Elevator Problem
o If accelerating upwards, you feel heavier
o If accelerating downwards, you feel lighter
Left Picture
o FN is your supporting
Force(Normal Force)
o FG=FN
Ο΄
Ο΄
Fg
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Right Picture(Color Coded)
o Fg(Weight)
o F⊥(Perpendicular to Inline)= mgcosΟ΄
o 𝐹𝑓 = πœ‡πΉπ‘ (πœ‡ = πΆπ‘œπ‘’π‘“π‘“π‘–π‘π‘Žπ‘›π‘‘ π‘œπ‘“ πΉπ‘Ÿπ‘–π‘π‘‘π‘–π‘œπ‘›)
 Friction opposes Motion
o FN=F⊥
o FP=mgsinΟ΄ (parallel to incline; always goes down hill)
Object at rest or moving at constant Velocity have a Net force of ZERO
Exam 3
Circular Motion
o Centripetal Force: Inward Force Needed to maintain circular motion
o 𝐹𝑐 =
π‘šπ‘£ 2
π‘Ÿ
ο‚· Centripetal Acceleration: The change in direction produced by a central force
o
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𝑣2
π‘Ÿ
The centripetal force is not a special kind of force; therefore never label a force on a free-body-diagram
as ‘centripetal’. The centripetal force is provided by the component of the force that is directed
towards the center of the circular path e.g. friction, tension, gravity, normal, etc.
Minimum Speed to go around once
o 𝑣 = √π‘Ÿπ‘”
Vertical Circle
o Top=Light
o Bottom=Heavy
Work
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Definition: The product of the displacement and the component of the force in the direction of the
displacement.(Units-Joules)
o π‘Š =𝐹×π‘₯
o The “F” is the Sum of the Forces
o “F” and “x” must go in the same direction
ο‚· Work and Energy and Scalar Quantities
ο‚· Work/ Energy Theorem
o π‘Š = βˆ†πΈ
ο‚· Graph of Force and Distance
o Area underneath is the work done
ο‚· Spring Force
o 𝐹𝑠 = π‘˜π‘₯
o K=Spring Constant
o X=distance stretched
Potential Energy
Kinetic Energy
2
1
π‘ˆπ‘’ = ⁄2 π‘˜π‘₯ ---Spring Stretched
𝐾 = 1⁄2 π‘šπ‘£ 2
π‘ˆπ‘” = π‘šπ‘”βˆ†π‘¦---Vertical
ο‚· Pendulum Problem
o π‘π‘œπ‘ πœƒ =
β„“−βˆ†π‘¦
β„“
ο‚· Positive and Negative Work
o Force acting on an object has the same direction as displacement = + W
o Force acting on an object has the opposite direction as displacement = -W
ο‚· Mechanical Energy= Constant!!
o If object is above the zero line of Potential Energy, then include Potential Energy
o If object is in motion at the point, then include kinetic Energy
o If object is a spring, then use only equations related to spring
 𝑀𝐹 = 𝐹𝑓 ∗ π‘₯
ο‚· DO NOT NEED MASS ALL THE TIME
Power
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Definition: The rate at which work is done
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𝑃=
π‘Š
𝑑
Exam 4
Newton’s Universal Law of Energy
𝐹𝑔 = 𝐺(
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π‘š1 π‘š2
)
π‘Ÿ2
r = distance apart from the center(m1 and m2)
Gravity= Force between objects
Every mass attracts other masses
G=6.67*10-11 Nm2/(kg)2
Kepler’s Law
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First Law
o Planets Revolve around the sun in ellipsis’s
Second Law
o “Law of equal areas”
o Speeds of the planets in their orbits
Third Law
o 𝑔=
𝐺𝑀
π‘Ÿ2


g = acceleration on any planet
M= Mass of object in “?”
πΊπ‘š
o 𝑣=√


o 𝑇2 =
π‘Ÿ
v = orbital speed
m= mass of “stationary object”
4πœ‹2 π‘Ÿ 3
𝐺𝑀
 T=Period(Sec.)
 r = meters
 M= stationary object
 Solar System Constant =
4πœ‹2
𝐺𝑀
Momentum
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𝑃⃗ = π‘šπ‘£
o P=momentum= kg(m/s)
o Write Positive or Negative Sign to show specific direction because it is a vector
βˆ†π‘ƒ
βƒ—βƒ—βƒ—βƒ—βƒ—βƒ—βƒ—
𝐹
𝑛𝑒𝑑 =
𝑑
o A force is the rate momentum changes
o Force get bigger when time gets smaller
Energy
Momentum
π‘Š = βˆ†πΈ
π‘Š =𝐹×π‘₯
Area under graph for Force-Displacement is work
πΌπ‘šπ‘π‘’π‘™π‘ π‘’ = βˆ†π‘ƒ
𝐼 = 𝐹𝑑
Area under Force-Time Graph is Implulse
Newton’s Third Law
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“For every action, there is an equal and opposite reaction”
How to formulate the Construction of Momentum
o
o
o
βƒ—βƒ—βƒ—
βƒ—βƒ—βƒ—βƒ—2
𝐹1 = −𝐹
βˆ†π‘ƒ1 = −βˆ†π‘ƒ2
βˆ†π‘ƒ1 + βˆ†π‘ƒ2 =0
o ∑ 𝑃𝑖 = ∑ 𝑃𝑓
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Inelastic Collision-Any collision where Ki>Kf
Elastic Collision- A collision that conserves Kinetic Energy --- NEVER ASSUME
Momentum is conserved in all collision systems. Kinetic energy is conserved only in elastic collisions.
Ballistic Pendulum
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K’=Ug
Find v’
Plug into the Construction of Momentum to find mass of bullet
This is one example of the many they can give you
Elastic Collision
ο‚· 𝑣2′ = (
2π‘š1
π‘š1 +π‘š2
π‘š1 −π‘š2
ο‚· 𝑣1′ = (
π‘š1 +π‘š2
) 𝑣1′
) 𝑣1
ο‚· One that is moving=m1
ο‚· One that is not=m2
Exam 5
Fluid
 𝑃=

𝐹
𝐴
=
𝑁
π‘š2
= π‘ƒπ‘Ž---Not a Vector. It is a scalar quantity.
𝑃𝑉 = 𝑛𝑅𝑇 --- Can only use two units
οƒ˜ Pa & m3
οƒ˜ Atm & L
 𝑃𝑓 = πœšπ‘“ π‘”β„Ž --- Pressure of a fluid
οƒ˜ Fluid pressure is independent of the shape or area of the container
 Density 𝜚 =
π‘š
𝑉
 Gauge Pressure = Pf --- Pressure only by fluid
 Absolute pressure is equal to the gauge pressure plus the atmospheric pressure
 Buoyant Force is upwards(against gravity) βƒ—βƒ—βƒ—βƒ—
𝐹𝐡 = πœšπ‘“ 𝑔𝑉𝑠
οƒ˜ VS= Volume of Object Submerged
οƒ˜ It is a vector
οƒ˜ Definition: Weight of Fluid displaced by Object
 Please Note that you can think of 𝐹𝑔 = πœšπ‘œ 𝑔𝑉𝑇
οƒ˜
Ο±o= density of object
Dynamic Fluids
 𝐴1 𝑣1 = 𝐴2 𝑣2 --- Equation of Continuity
οƒ˜ Flow Rate
 𝐴1 𝑣1
 π‘š2 ∗ π‘š⁄𝑠


π‘š3
𝑠
𝑉⁄
𝑠
 Bernoulli's Equation: The net work done on a fluid is equal to the changes in kinetic and potential energy of
the fluid in terms of quantities per volume.
οƒ˜ 𝑃1 + 1⁄2 πœšπ‘£1 2 + πœšπ‘”π‘¦1 = 𝑃2 + 1⁄2 πœšπ‘£2 2 + πœšπ‘”π‘¦2
οƒ˜ Any Time fluid is exposed to air the Pressure = 1 atm
οƒ˜ If the distances between the two fluids are very close, then they can be set to zero
οƒ˜ If water is leaking then you can find velocity using …. 𝑣 = √2𝑔𝑦
Exam 6-ThermoDynamics
Thermo expansion
 Increase of a temperature on object
 Expanding of metals at a rate
Linear Expansion
βˆ†πΏ =⋉ 𝐿0 βˆ†π‘‡
Coefficient of Linear
Expansion 1/co or oc-1
Ideal Gas Law
1. 𝑃𝑉 = 𝑛𝑅𝑇
a. n=moles
b. Value of R
i. 8.31 J/(mol*K)
ii. 0.0821 (atm*L)/(mol*K)
c. T --- Always use Kelvin for temp Scale
i. ___oK=___oC+273
2. 𝑛 ∗ 𝑁𝐴 = 𝑁
oC!!!
a. n = # of moles
b. NA = Avogadro’s # = 6.022 *1023
c. N = # of Molecules
3. 𝑃𝑉 = 𝑁𝓀𝑇
a. 𝓀 = Boltzmann’s Constant = 1.38 * 10-23 J/K
Kinetic Theory
 Kinetic theory relates the average kinetic energy of the molecules in a gas to the temperature of the gas in
Kelvin
𝑃=
1𝑁
3𝑉
[π‘šπ‘£Μ… 2 ] same as 𝑃 =
2𝑁
3𝑉
Μ…
𝐾
Μ… = 3⁄ 𝓀𝑇
𝐾
2
 π‘£π‘Ÿπ‘šπ‘  = √
3𝓀𝑇
π‘š
οƒ˜ m = mass of single molecule
οƒ˜ r.m.s= root mean square
οƒ˜ i.e. O2 = 16 g/mol (Periodic Table) * 2(diatomic) = 21 g/mol οƒ  Then divide by 1000 οƒ  then divide by NA
οƒ  Changed to Kg which is the value you need for “m”
Thermal Energy/ Law of Thermodynamics
 βˆ†π‘ˆ = 3⁄2 π‘π“€βˆ†π‘‡
οƒ˜ Internal Energy of Gas
 First Law of Thermodynamics
οƒ˜ βˆ†π‘ˆ = βˆ†π‘„ − π‘Š
οƒ˜ Work is done ON the System
οƒ˜ π‘Š = π‘ƒβˆ†π‘‰
 The Sign is Important so always put a “+” or “-“
P-V Diagrams
(1) Isobaric Process- Process when Pressure is constant
(2) Isometric(Isochoric) Process – Occurs at Constant Volume
a. βˆ†π‘ˆ = βˆ†π‘„
(3) Isothermal Process – Constant Temperature
a. Everywhere, V1P1=P2V2
𝑉𝑓
b. π‘Š = 𝑛𝑅𝑇 ln ( )
𝑉
𝑖
𝑉
c. π‘Š = 𝑃𝑉 ln ( 𝑓⁄𝑉 ) --- Same as above
𝑖
d. βˆ†π‘„ = π‘Š
(4) Adiabatic Pressure
a. βˆ†π‘„ = 0
b. βˆ†π‘ˆ = −π‘Š
(5) Complete Cycle
a.
b.
c.
d.
Total for delta U = 0
Total for delta Q = W
Total for W= “+”
Pay Attention to Direction
Carnot Engine
π‘„β„Ž = 𝑄𝑐 + π‘Š
 Carnot cycles involve only isothermal and adiabatic processes. To determine the efficiency use the Kelvin
temperatures of the reservoirs.
 Carnot Engine = The “Perfect” Cycle
 Efficiency of any engine πœ€ =
π‘Š
π‘„β„Ž
=1−
𝑄𝑐
π‘„β„Ž
 Efficiency of Carnot (maximum Efficiency) πœ€ = 1 −
Watt = (J/S) = Energy/Time = P
(Didn’t know where to put this)
Negative Work (Gas Does the Work)
(1) π‘Š = −(𝑃Δ𝑉)
(2) Δπ‘ˆ = Δ𝑄 + π‘Š
V
(3) W = −nRT ln ( f⁄V )
i
Entropy
 Basic measure of “disorder”
 Entropy of the universe is always “+”
 Δ𝑠 =
Δ𝑄
𝑇
οƒ˜ s = entropy
οƒ˜ Q= change in entropy
οƒ˜ T= Kelvin

𝑄𝑐
𝑇𝑐
=
𝑄𝐻
𝑇𝐻
𝑇𝑐
π‘‡β„Ž
1Carnot Cycle-Only Adiabatic
and Isothermal
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