Comprehensive Review Comprehensive Review a) Exam information b) What kind of questions? c) Review
Midterm 3 Exam in-class Average = 5.1/12 Average = 57% (normalized to 9) The score for Midterm 3 will be calculated with the following formula:
Final Exam Review the following material homework problems. video pre-lectures/textbook. Lecture slides Unit Main Points Multiple choice…but show your work and justification. Mostly Calculations…”step by step” Some Conceptual questions…like checkpoint problems. Bring calculators and up to ten sheets of notes. It is best to prepare your own hand-written notes! Derived Equations may be helpful…(e.g. projectile motion)
Kinematics Force Energy Conservation Laws Collisions Rotations What we covered… Kinematics Description of Motion Force Dynamics-how objects change velocity Energy Kinetic and Potential Conservation Laws Momentum and Energy Collisions Elastic and In-elastic Rotations Torque/ Angular Momentum/Statics
Problem Solving Techniques Visualize/Diagram “Sketch” problem Identify variables, input and what we are trying to solve Free-body diagrams Express in Mathematical Equations Scalars-1d Vectors-2d,3d Break into components System of n-equations with n-unknowns Use Mathematical tools to solve: Quadratic Equation Vector operations Trigonometry Conceptual Understanding Does answer make sense?
Potential Problem Topics Projectile Motion Relative Motion - 2d Uniform Circular Motion Forces Weight (near earth) Gravitational (satellite) Springs Normal Force Tension Friction Free-Body Diagrams Work-Kinetic Energy Potential Energy Center of Mass Conservation of Momentum Collisions In-elastic Elastic Rotations Kinematics Dynamics Statics Moment of Inertia Torque Angular Momentum
Relevant Formulae
Relevant Formulae
Kinematics
Hyperphysics Motion Displacement vs timet Velocity vs timet Acceleration vs timet
Hyperphysics Motion
1d-Kinematic Equations for constant acceleration Basic Equations to be used for 1d – kinematic problems. Need to apply to each object separately sometimes with time offset When acceleration changes from one constant value to another say a=0 The problem needs to be broken down into segments
Ballistic Projectile Motion Quantities Initial velocity speed,angle Maximum Height of trajectory, h=ymax “Hang Time” Time of Flight, tf Range of trajectory, D Height of trajectory at arbitrary x,t
Derived Projectile Trajectory Equations Maximum height Time of Flight (“Hang Time”) Range of trajectory Height of trajectory as f(t) , y(t) Height of trajectory as f(x), y(x)
Relative Motion in 2 Dimensions Direction w.r.t shoreline Speed relative to shore
Uniform Circular Motion
Uniform Circular Motion Constant speed in circular path Acceleration directed toward center of circle What is the magnitude of acceleration? Proportional to: Speed time rate of change of angle or angular velocity v = wR
Dynamics
Inventory of Forces Weight Normal Force Tension Gravitational Springs …Friction
http://hyperphysics.phy-astr.gsu.edu/hbase/N2st.html#c1
m2 1) FBD N T m2 g f T m1 m1 m2g m1g 22
m2 N T m2 f T m1 m2g N = m2g m1g m1g – T = m1a T – m m2g = m2a 1) FBD 2) SF=ma N T m2 g f T m1 m1 m2g N = m2g m1g T – m m2g = m2a m1g – T = m1a add m1g – m m2g = m1a + m2a m1g – m m2g a = m1 + m2 23
m2 N T m2 f T m1 m2g m1g m1g – T = m1a T = m1g – m1a 1) FBD 2) SF=ma g m1g – m m2g T = m1g – m1a a = m1 + m2 T is smaller when a is bigger 24
Gravitation Problems…too!
Be careful what value you use for r Be careful what value you use for r !!! Should be distance between centers of mass of the two objects
Work-Kinetic Energy Theorem The work done by force F as it acts on an object that moves between positions r1 and r2 is equal to the change in the object’s kinetic energy: But again…!!!
Energy Conservation Problems in general For systems with only conservative forces acting Emechanical is a constant
(otherwise objects velocity is constant) Determining Motion Force Unbalanced Forces acceleration (otherwise objects velocity is constant) Determine Net Force acting on object Use kinematic equations to determine resulting motion Energy Total Energy Motion, Location Work Conservative forces Motion from Energy conservation
Friction “It is what it has to be.”
Block
Work & Kinetic Energy
Example Problem
Potential Energy
Example Problems
Example: Pendulum h h Conserve Energy from initial to final position.
Gravitational Potential Problems conservation of mechanical energy can be used to “easily” solve problems. Define coordinates: where is U=0? Add potential energy from each source. as
Collisions Center of Mass Conservation of Momentum Inelastic collisions Elastic Collisions Impulse and Reference Frames Multiple particles, Solid Objects Isolated system, No external force Non-conservative internal force Conservative internal force Individual Particle changes momentum due to Force acting over a given duration Favg = DP/Dt
Systems of Particles
Example Problem
Collisions
Example Problem
Example Problem :
Impulse
|Favg | = |DP | /Dt = 2mv cosq /Dt
Rotations Rotational Kinematics Moment of Inertia Torque Rotational Dynamics Rotational Statics Angular Momentum Description of motion about a center of mass Resistance to changes in angular velocity Force applied at a lever arm resulting in angular acceleration Newton’s 2nd law for rotations How to ensure stability Vector Quantity describing object(s) rotation about an axis
Rotational Kinematics
Rotational Dynamics
Example Problem
Example Problem
Work & Energy (rotations)
Example Problem
Statics
Statics Problems
Example Problem
Angular Momentum
Example Problem
Relevant Formulae
Relevant Formulae