AP Physics B Review --- ASHWIN JACOB Exam 1 Kinematics ο· ο· ο· 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) π£Μ = 2) π£Μ = 3) πΌ = βπ βπ‘ ππ +π£π 2 Δv Δt = ππ −π£π π‘ 4) π₯π = π₯π + π£π π‘ + 1⁄2 ππ‘ 2 5) π£π 2 = π£π 2 + 2πΔπ₯ ο· ο· 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 ο· Shortcut for velocity of free-falling object π£ = √2πβπ¦ ο· Analyzing Graphs o Area of Graph is the distance o Graph B ο§ 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**** ο· Vectors- Quantities that require both size(magnitude) and direction o Velocity, Displacement, and Force Scalars-Magnitude Only o Volume, Mass, Distance, Speed Vector Equations ο· ο· o π₯ = π × cos π o π¦ = π × sin π o ∑ π₯ = π΄π₯ − π΅π₯ β = √∑ π₯ 2 + ∑ π¦ 2 o π o π = tan−1 ( ο· ∑π¦ ∑π₯ ) Vector Example o → =50m @ 40o N of E A o → = 20π @ 30π π ππ π π΅ 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 ο· 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 β = π΄ + (−π΅ β) ο§ π΄−π΅ ο§ Just the opposite of B = Same Angle, Same Meter, Different Direction Two-Dimension Kinematics ο· The horizontal and vertical motions of a projectile are independent of one another ο· Changed Equations o π¦π = π¦π + π£π π‘ + 1⁄2 ππ‘ 2 o π₯ = π£Μ π‘ o Still Need to consider the angles Newton’s First Law (Law of Inertia) ο· ο· ο· 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 πΉπππ‘ = ππ o Two things to Remember ο§ Vector Equation ο§ Net Force and Acceleration MUST have the same direction!!! ο· ο· FN ο· ο· o πΉ = ππ (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 ο· Right Picture(Color Coded) o Fg(Weight) o F⊥(Perpendicular to Inline)= mgcosΟ΄ o πΉπ = ππΉπ (π = πΆπππππππππ‘ ππ πΉππππ‘πππ) ο§ 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 πΉπ = ππ£ 2 π ο· Centripetal Acceleration: The change in direction produced by a central force o ο· ο· ο· π£2 π 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 π£ = √ππ Vertical Circle o Top=Light o Bottom=Heavy Work ο· Definition: The product of the displacement and the component of the force in the direction of the displacement.(Units-Joules) o π =πΉ×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 = βπΈ ο· Graph of Force and Distance o Area underneath is the work done ο· Spring Force o πΉπ = ππ₯ o K=Spring Constant o X=distance stretched Potential Energy Kinetic Energy 2 1 ππ = ⁄2 ππ₯ ---Spring Stretched πΎ = 1⁄2 ππ£ 2 ππ = ππβπ¦---Vertical ο· Pendulum Problem o πππ π = β−βπ¦ 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 ο§ π€πΉ = πΉπ ∗ π₯ ο· DO NOT NEED MASS ALL THE TIME Power ο· Definition: The rate at which work is done ο· π= π π‘ Exam 4 Newton’s Universal Law of Energy πΉπ = πΊ( ο· ο· ο· ο· π1 π2 ) π2 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 ο· ο· ο· 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 π= πΊπ π2 ο§ ο§ g = acceleration on any planet M= Mass of object in “?” πΊπ o π£=√ ο§ ο§ o π2 = π v = orbital speed m= mass of “stationary object” 4π2 π 3 πΊπ ο§ T=Period(Sec.) ο§ r = meters ο§ M= stationary object ο§ Solar System Constant = 4π2 πΊπ Momentum ο· ο· πβ = ππ£ o P=momentum= kg(m/s) o Write Positive or Negative Sign to show specific direction because it is a vector βπ βββββββ πΉ πππ‘ = π‘ o A force is the rate momentum changes o Force get bigger when time gets smaller Energy Momentum π = βπΈ π =πΉ×π₯ Area under graph for Force-Displacement is work πΌπππ’ππ π = βπ πΌ = πΉπ‘ Area under Force-Time Graph is Implulse Newton’s Third Law ο· ο· “For every action, there is an equal and opposite reaction” How to formulate the Construction of Momentum o o o βββ ββββ2 πΉ1 = −πΉ βπ1 = −βπ2 βπ1 + βπ2 =0 o ∑ ππ = ∑ ππ ο· ο· ο· 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 ο· ο· ο· ο· 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· π£2′ = ( 2π1 π1 +π2 π1 −π2 ο· π£1′ = ( π1 +π2 ) π£1′ ) π£1 ο· One that is moving=m1 ο· One that is not=m2 Exam 5 Fluid οΆ π= οΆ πΉ π΄ = π π2 = ππ---Not a Vector. It is a scalar quantity. ππ = ππ π --- Can only use two units ο Pa & m3 ο Atm & L οΆ ππ = ππ πβ --- Pressure of a fluid ο Fluid pressure is independent of the shape or area of the container οΆ Density π = π π οΆ Gauge Pressure = Pf --- Pressure only by fluid οΆ Absolute pressure is equal to the gauge pressure plus the atmospheric pressure οΆ Buoyant Force is upwards(against gravity) ββββ πΉπ΅ = ππ πππ ο VS= Volume of Object Submerged ο It is a vector ο Definition: Weight of Fluid displaced by Object οΆ Please Note that you can think of πΉπ = ππ πππ ο Ο±o= density of object Dynamic Fluids οΆ π΄1 π£1 = π΄2 π£2 --- Equation of Continuity ο Flow Rate ο§ π΄1 π£1 ο§ π2 ∗ π⁄π ο§ ο§ π3 π π⁄ π οΆ 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. ο π1 + 1⁄2 ππ£1 2 + πππ¦1 = π2 + 1⁄2 ππ£2 2 + πππ¦2 ο Any Time fluid is exposed to air the Pressure = 1 atm ο If the distances between the two fluids are very close, then they can be set to zero ο If water is leaking then you can find velocity using …. π£ = √2ππ¦ Exam 6-ThermoDynamics Thermo expansion οΆ Increase of a temperature on object οΆ Expanding of metals at a rate Linear Expansion βπΏ =β πΏ0 βπ Coefficient of Linear Expansion 1/co or oc-1 Ideal Gas Law 1. ππ = ππ π 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. π ∗ ππ΄ = π oC!!! a. n = # of moles b. NA = Avogadro’s # = 6.022 *1023 c. N = # of Molecules 3. ππ = πππ a. π = Boltzmann’s Constant = 1.38 * 10-23 J/K Kinetic Theory οΆ Kinetic theory relates the average kinetic energy of the molecules in a gas to the temperature of the gas in Kelvin οΆπ= 1π 3π [ππ£Μ 2 ] same as π = 2π 3π Μ πΎ Μ = 3⁄ ππ οΆπΎ 2 οΆ π£πππ = √ 3ππ π ο m = mass of single molecule ο r.m.s= root mean square ο i.e. O2 = 16 g/mol (Periodic Table) * 2(diatomic) = 21 g/mol ο Then divide by 1000 ο then divide by NA ο Changed to Kg which is the value you need for “m” Thermal Energy/ Law of Thermodynamics οΆ βπ = 3⁄2 ππβπ ο Internal Energy of Gas οΆ First Law of Thermodynamics ο βπ = βπ − π ο Work is done ON the System ο π = πβπ οΆ 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. βπ = βπ (3) Isothermal Process – Constant Temperature a. Everywhere, V1P1=P2V2 ππ b. π = ππ π ln ( ) π π π c. π = ππ ln ( π⁄π ) --- Same as above π d. βπ = π (4) Adiabatic Pressure a. βπ = 0 b. βπ = −π (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 πβ = ππ + π οΆ Carnot cycles involve only isothermal and adiabatic processes. To determine the efficiency use the Kelvin temperatures of the reservoirs. οΆ Carnot Engine = The “Perfect” Cycle οΆ Efficiency of any engine π = π πβ =1− ππ πβ οΆ Efficiency of Carnot (maximum Efficiency) π = 1 − Watt = (J/S) = Energy/Time = P (Didn’t know where to put this) Negative Work (Gas Does the Work) (1) π = −(πΔπ) (2) Δπ = Δπ + π V (3) W = −nRT ln ( f⁄V ) i Entropy οΆ Basic measure of “disorder” οΆ Entropy of the universe is always “+” οΆ Δπ = Δπ π ο s = entropy ο Q= change in entropy ο T= Kelvin οΆ ππ ππ = ππ» ππ» ππ πβ 1Carnot Cycle-Only Adiabatic and Isothermal