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Final Exam Review (Day 1)

Final Exam Review (Day 1). Energy Lecture Review Kinetic & Potential Energy Net Work (W net = F net x = F net cos ) Work-Kinetic Energy Theorem

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Page 1: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Final Exam Review (Day 1)

Page 2: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Energy Lecture Review Kinetic & Potential Energy Net Work (Wnet = Fnet x = Fnet cos ) Work-Kinetic Energy Theorem (W = KE) Conservation of Energy (KEi + PEi = KEf +

PEf)

Problem Review (Group Problems) Energy Net Forces

Page 3: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Potential Energy Stored Energy In Which An Object May

Use To Perform Work On Another Object Gravitational Potential (PE = mgh) Elastic Potential (PE = ½ kx2) Chemical Potential (PE = nCvT)

Kinetic Energy Energy Achieved By An Object In Motion Kinetic Energy (KE = ½ mv2)

Page 4: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Work Done On An Object With Multiple Forces Is The Net Work

For A Net Force Applied At An Angle, The Net Work Is The Product Of The Component Of Force In The Direction Of Motion & Its Displacement

Wnet = Fnet x = Fnet cos

Page 5: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Work Done On (Net External Force) An Object Results In A Change In The Object’s Kinetic Energy Work = Force x Displacement or W = Fx Work-KE Theorem Is Equivelent To The

Following Expression:

W = KEf – KEi = ½ mvf2 – ½ mvi

2

Page 6: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Total Mechanical Energy (ME = KE + PE) Of An Object Remains Constant As The Object Moves Assume No Net Work Done By External Forces

(e.g. Friction, Air Resistance, Pressure, etc.)

MEi = MEf

KEi + PEi = KEf + PEf

Page 7: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

The Drawing Shows A Boat Being Pulled By Two Locomotives Through A Canal Of Length 2.00 km. The Tension In Each Cable Is 5.00 x 103

N, And = 20.0o.

What Is The Net Work Done On The Boat By The Two Locomotives?

Page 8: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

A 0.075 kg Arrow Is Fired Horizontally. The Bowstring Exerts An Average Force Of 65 N On The Arrow Over A Distance Of 0.90 m.

With What Speed Does The Arrow Leave The Bow?

Page 9: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

A Cyclist Approaches The Bottom Of A gradual Hill AT A Speed Of 11 m/s. The Hill Is 5.0 m High, And The Cyclist Estimates That She Is Going Fast Enough To Coast Up And Over It Without Peddling.

Ignoring Air Resistance And Friction, Find The Speed AT Which The Cyclist Crests The Hill.

Page 10: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Final Exam Review (Day 2)

Page 11: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Momentum Lecture Review Impulse (I = Fnett = p = pf – pi) Conservation Of Momentum (Pi = Pf) Collisions (Elastic & Inelastic) Circular Motion (ac = vt

2/R) Gravitation (Fg = Gm1m2/d2)

Problem Review (Group Problems) Momentum Collisions Circular Motion

Page 12: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

When A Large Force Acts on An Object For A Sufficient Amount Of Time, Their Product Is The Impulse Of The Force

I = Fnett

The Object Will Thusly Experience A Change In Velocity (Or Change In Momentum) As Shown From Newton’s 2nd Law:

I = Fnett = p = pf – pi

Page 13: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

The Total Linear Momentum Of An Isolated System Remains Constant An Isolated System Is One For Which The

Vector Sum Of The External Forces Acting On The System Is Zero

Pi = Pf

mv1i + mv2i = mv1f + mv2f

Page 14: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Elastic Collision Is One In Which The Total KE Of The System After The Collision Is Equal To The Total KE Before The Collision

Inelastic Collision Is One In Which The Total KE Of The System After The Collision Is Not Equal To The Total KE Before The Collision

Page 15: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Uniform Circular Motion Is The Motion Of An Object Traveling At A Constant (Uniform) Speed On A Circular Path Even Though An Object In Circular Motion

Has A Constant Velocity (VT) It Experiences An Acceleration Toward The Center Of The Circular Path

ac = vt2/R

Page 16: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Objects With Mass Are Seemingly Attracted To Each Other Through The Gravitational Force

Fg = Gm1m2/d2

G Is The Gravitational Constant And Has An Experimentally Determined Value of:

G = 6.67 x 10-11 Nm/kg2

Page 17: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

During A Storm, Rain Comes Straight Down With A Velocity Of vo = -15 m/s And Comes To Rest After Impacting The Car. If The Rain Drops Have A Mass Of 0.060 kg & It Takes 1.0s To Come To A Rest, What Is The Force Exerted By The Rain On The Car Roof?

If Hail Fell Instead Of Rain, Would The Force On The Roof Be Smaller Than, Equal To , Or Greater Than That Of The Raindrop?

Page 18: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

A Ball Of Mass m1 = 0.250 kg And Velocity v1i = +5.0 m/s Collides Head-on With A Ball Of Mass m2 = 0.800 kg That Is Initially At Rest. No External Forces Act On The Balls.

If The Collision Is Elastic, What Are The Velocities Of The Balls After The Collision?

Page 19: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

How Long Does It Take A Plane, Traveling At A Constant Speed Of 110 m/s, To Fly Once Around A Circle Whose Radius Is 2850 m?

Page 20: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Final Exam Review (Day 3)

Page 21: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Kinematics Lecture Review Displacement, Velocity & Acceleration Speed Versus Velocity Graphical Models Of Motion Kinematic Equations Freefall 2-D Kinematics

Horizontal Projectile Motion Projectile Motion @ Angle

Problem Review (Group Problems) 1-D Kinematics 2-D Kinematics

Page 22: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Displacement Is A Vector That Points From An Object’s Initial Position Toward Its Final Position (Shortest Distance Between Two Points)

x = xf - xi

Velocity Is Defined As The Displacement (Change In Position) Of An Object Divided By The Change In Time

v = x/t

Acceleration Is The Change In Velocity Of An Object Over The Change In Time

a = v/t

Page 23: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

What Is Speed? Speed Is An Average Velocity If I Asked How Fast You Drove From Home

To School Today What Would You Say?

What About Velocity Then? Velocity Is Instantaneous, It Changes From

One Second To The Next Watch Your Speedometer Next Time You’re

Driving!

Page 24: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Position Versus Time (x versus t)

Velocity Versus Time (v versus t)

Slope = x/t = Velocity

Slope = v/t = Acceleration

t

t

x

v

Page 25: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Kinematics is the study of objects’ motion at constant acceleration

There are 4 kinematic equations

Use these to solve all 1-D and 2-D motion problems!

Page 26: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Equation Formula Relationship

#1 Velocity to Time

#2 Displacement to Time

#3 Velocity to Displacement

#4 Average Velocity

tavv if

2

2

1tatvx i

xavv if 222

t

xvvv if

2

Page 27: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Freefalling Bodies Move Freely Under The Influence Of Gravity ONLY!

The Acceleration Of An Object In Freefall Is ALWAYS The Acceleration Of Gravity

ag = -9.81 m/s2

Use Kinematic Equations To Solve Freefall Problems What Is The Acceleration Of An Object

Thrown Upwards? What Is The Velocity Of An Object At The

Peak Of Its Motion?

FREEFALL

Page 28: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Projectile Motion Horizontal Projectile Motion Projectile Motion At An Angle

Problem Solving Method First Commandment Of Physics (Keep

X & Y Directions Separate) Solve For Time In Y-Direction Using A

Kinematic Equation Use Vix = x/t In The X-Direction

Page 29: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

What Is The Acceleration AtThe Following Points:

a). 0 to 5 s b). 5 to 15 s c). 15 to 20 s

Page 30: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

A Baseball Player Hits A Triple And Ends Up On Third Base. A Baseball “Diamond” Is A Square, Each Side Of Length 27.4 m. What is The Magnitude Of His Displacement?

If The Same Baseball Player Rounds 2nd Base With A Velocity Of 10 m/s & Slides To A Stop At 3rd Base, What Is His Deceleration From 2nd To 3rd?

Page 31: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

A Quarterback Throws A Pass To A Receiver, Who Catches It At The Same Height As The Pass Is Thrown. The Initial Velocity Of The Ball Is 15.0 m/s, At An Angle Of 25.0o Above The Horizontal. What Is The Horizontal Component Of The Ball’s Velocity When The Receiver Catches It?

Page 32: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

PROBLEM #4: 2-D KINEMATICS

Given The Last Problem, How Far Did The Receiver Have To Run Before Making The Catch?

Page 33: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Final Exam Review (Day 4)

Page 34: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Dynamics Lecture Review Force Types (4 Major Forces) Newton’s Laws Of Motion

1st Law (Freebody Diagrams) 2nd Law (F = Fnet = ma) 3rd Law (F12 = -F21)

Problem Review (Group Problems) Net Force Newton’s Second Law I Newton’s Second Law II

Page 35: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

An Object With Mass (Takes Up Space) In The Presence Of Gravity Has Weight.

W = mg Any Object In Contact With A Surface Experiences

A Force Normal To The Surface Called The Normal Force (FN)

An Applied Force (Mechanical or Electrical) Is One That Is Applied To An Object Causing It To Move (FA)

The Resistive Force Acting On An Object In Contact With Another Surface Is The Force Due To Friction Static Friction (Fs = sFN) Kinetic Friction (Fk = kFN)

Page 36: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Fk

W

FN

Page 37: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Draw The Freebody (The Object Separated From Its Surroundings)

Draw Relevant Forces Acting On The Freebody From The Center Of The Object Does The Body Have Mass In The

Presence Of Gravity? Is The Object In Contact With A Surface?

If Yes, Is The Contact Surface Frictionless or Is Friction Present?

Is There An Applied Force?

Page 38: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Second Law: The Net Force (Fnet = F) Acting On An Object Will Cause The Object To Accelerate (Motion)

F = ma Add Forces In Different Directions Vectorally

Fnet 2 = Fx2 + Fy

2 (Magnitude)

Tan () = Fy/Fx (Direction)

Page 39: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

First LawAn Object In Motion Will Stay In Motion

Until Acted Upon By An External Net ForceAn Object At Rest Will Remain At Rest Until

Acted Upon By An External Net Force Third Law

Two Objects In Contact Will Apply Forces Equal In Magnitude But Opposite In Direction

F12 = -F21

Page 40: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

A Person With A Blackbelt In Karate Has A Fist That Has A Mass Of 0.70 kg. Starting From Rest, This Fist Attains A Velocity Of 8.0 m/s In 0.15 s. What Is The Magnitude Of The Average Net Force Applied To The Fist To Achieve This Level Of Performance?

Page 41: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Two Forces, F1 & F2, Act On The 5.0 kg Block Shown In The Drawing. The Magnitudes Of The Forces Are F1 = 45.0 N And F2 = 25.0 N. What Is The Horizontal Acceleration (Magnitude & Direction) Of The Block?

Page 42: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

A 92 kg Baseball Player Slides Into Second Base. The Coefficient Of Kinetic Friction Between The Player And The Ground Is k = 0.61.

a). What Is The Magnitude Of The Frictional Force?

b). If The Player Comes To Rest After 1.2 s, What Is His Initial Speed?

Page 43: Final Exam Review (Day 1).  Energy Lecture Review  Kinetic & Potential Energy  Net Work (W net = F net  x = F net cos  )  Work-Kinetic Energy Theorem

Given The Following Atwood Machine With Masses M and m, Determine The Acceleration Of Mass m.

m