Force Summary

Types of Forces

Listing All Forces On An Object: Long-Range Forces

  • Weight:

    • Consider weight unless it's negligible.

    • It is negligible if the object is very light compared to other large forces.

    • Weight is relevant if the object is not rolling down, sliding down, sagging, or falling.

  • Electric or Magnetic Forces:

    • Not typically covered in this class.

    • Look for:

      • Electric Forces: Charged objects

      • Magnetic Forces: Charges, electric currents, bar magnets, iron, nickel, or cobalt.

  • Gravitational Force: Represented as Fg\vec{F}_g

Listing All Forces On An Object: Contact Forces

  • Identify Contact:

    • List every object the object of interest is touching.

  • Determine Force Types for Each Object in Contact:

    • Pulling: If a string, chain, or similar object is pulling, consider tension.

    • Touching Surfaces: Consider normal forces.

    • Sliding: Consider kinetic friction.

    • Rolling: Consider rolling friction and if it has traction

    • Touching a Fluid:

      • Buoyant force should be considered.

      • Buoyant force is negligible if the fluid has low density and the object is not very light.

    • Moving Through a Fluid:

      • Consider drag force.

      • Drag force is negligible if the object is moving slowly, is very heavy, or very small

  • Important Note:

    • No other forces exist besides those listed.

    • Objects must pass a "kick test" to ensure the forces are real.

  • Common Contact Forces:

    • Normal Force: FN\vec{F}_N

    • Tension: FT\vec{F}_T

    • Kinetic Friction: Fk\vec{F}_k

    • Static Friction: FS\vec{F}_S

    • Rolling Friction: FR\vec{F}_R

    • Buoyant Force: FB\vec{F}_B

    • Drag Force: FD\vec{F}_D

Clicker Questions Breakdown

The following sections break down the clicker questions included in the transcript.

Clicker Question 14
  • Scenario: Boxes being pulled up a ramp.

  • Question: Which free body diagram best represents the forces on box A?

  • Correct Answer: C)

  • Forces Illustrated:

    • Fg\vec{F}_g (Gravitational Force)

    • FN\vec{F}_N (Normal Force)

    • FT\vec{F}_T (Tension)

Clicker Question 15
  • Scenario: Boxes being pulled up a ramp.

  • Question: Which free body diagram best represents the forces on box B?

  • Correct Answer: D)

  • Forces Illustrated:

    • FN\vec{F}_N (Normal Force)

    • Fg\vec{F}_g (Gravitational Force)

    • FT\vec{F}_T (Tension)

    • Fk\vec{F}_k (Kinetic Friction)

  • Additional Notes from the slide:

    • FT,rope on B\vec{F}_{T, rope \text{ on } B} represents the tension force by the rope on box B.

    • FN,floor on B\vec{F}_{N, floor \text{ on } B} represents the normal force by the ramp/floor on box B.

    • Fk,floor on B\vec{F}_{k, floor \text{ on } B} represents the kinetic friction force by the ramp/floor on box B.

Clicker Question 16
  • Scenario: Forces on a weight on a string as it swings back and forth.

  • Question: Which free body diagram best represents the forces on the weight?

  • Correct Answer: B)

  • Forces Illustrated:

    • Fg\vec{F}_g (Gravitational Force)

    • FT\vec{F}_T (Tension)

Clicker Question 17
  • Scenario: Forces acting on a person.

  • Question: Which free body diagram best matches the situation of the person?

  • Correct Answer: B)

  • Forces Illustrated:

    • FN\vec{F}_N (Normal Force)

    • Fg\vec{F}_g (Gravitational Force)

Newton's Laws of Motion

Slides Overview

  • Newton’s Third Law: Forces between Objects

  • Newton’s First Law:

    • Forces without acceleration

    • Lab 5: Net Force

  • Newton’s Second Law:

    • Forces with acceleration

    • Lab 6: Unbalanced Forces

Forces Between Objects: Newton’s Third Law

  • Basic Idea: When you push on something, it pushes back.

  • Common Phrasing: “Every action has an equal and opposite reaction.”

  • Better Phrasing: “For every force by A on B, B exerts a force back on A equally hard in the opposite direction.”

  • Newton’s Third Law (Equation): F<em>byAonB=F</em>byBonA\vec{F}<em>{by \, A \, on \, B} = -\vec{F}</em>{by \, B \, on \, A}

Newton’s Third Law on Free Body Diagrams

  • Labeling Convention: Each force in a free body diagram should end with “on [object]”.

  • Third Law Pairs: Pairs of forces are on different free body diagrams.

  • Examples discussed:

    • Box B:

      • Fg,EarthonB\vec{F}_{g, Earth \, on \, B}

      • FN,ramponB\vec{F}_{N, ramp \, on \, B}

      • FT,ropeonB\vec{F}_{T, rope \, on \, B}

      • FN,AonB\vec{F}_{N, A \, on \, B}

      • Fk,ramponB\vec{F}_{k, ramp \, on \, B}

      • FS,AonB\vec{F}_{S, A \, on \, B}

    • Box A:

      • Fg,EarthonA\vec{F}_{g, Earth \, on \, A}

      • FN,BonA\vec{F}_{N, B \, on \, A}

      • FS,BonA\vec{F}_{S, B \, on \, A}

Clicker Question 1 (Newton's Third Law Pairs)

  • Scenario: Books stacked on a table.

  • Question: Which of the following forces are Newton’s 3rd Law pairs?

  • Correct Answer: C) F<em>N,byAonB\vec{F}<em>{N, by \, A \, on \, B} & F</em>N,byBonA\vec{F}</em>{N, by \, B \, on \, A}

Clicker Question 2 (Number of Newton's Third Law Pairs)

  • Scenario: Three books stacked on a table.

  • Question: How many Newton’s 3rd Law pairs of normal forces would appear on the 3 FBD, one for each book?

  • Correct Answer: D) 3

Class Problem: Books on a Table (Part 1)

  • Problem: Three books (A, B, C with masses 0.5 kg, 1 kg, and 2 kg respectively) are stacked on a table.

  • Tasks:

    • Draw a properly labeled free body diagram for each book.

    • Identify Newton’s 3rd Law force pairs.

  • Key Insight: Newton’s Third Law force pairs are the same force, just flipped in direction.

  • Forces Identified:

    • Fg,EonA\vec{F}_{g,E \, on \, A}

    • Fg,EonB\vec{F}_{g,E \, on \, B}

    • Fg,EonC\vec{F}_{g,E \, on \, C}

    • FN,BonA\vec{F}_{N,B \, on \, A}

    • FN,AonB\vec{F}_{N,A \, on \, B}

    • FN,ConB\vec{F}_{N,C \, on \, B}

    • FN,BonC\vec{F}_{N,B \, on \, C}

    • FN,TonC\vec{F}_{N,T \, on \, C}

Clicker Question 3 (Semi Truck vs. Small Car Collision)

  • Scenario: A semi truck collides with a small car.

  • Question: Which force is greater?

  • Correct Answer: C) The two are equal.

  • Explanation: According to Newton's Third Law, the forces will always be equal, although the acceleration experienced by each vehicle will differ due to their different masses.

Net Force with Constant Velocity: Newton's 1st Law

Lab 5: Net Force (Part 1)

Newton’s First Law
  • Basic Idea: Objects don’t change velocity without a net force on them.

  • Common Phrasing: “An object in motion stays in motion unless acted upon by an external force.”

  • Better Phrasing: “If and only if there is no net force on an object, it has no acceleration.”

  • Equation: F<em>onA=0 if and only if a</em>A=0\sum \vec{F}<em>{on \, A} = 0 \text{ if and only if } \vec{a}</em>A = 0

    • FonA\sum \vec{F}_{on \, A} is the net force on a generic object “A”.

    • aA\vec{a}_A is the acceleration of “A”.

Clicker Question 4 (Puck Sliding on Ice)

  • Scenario: A puck slides across a slick ice rink at a constant speed, in a straight line.

  • Question: What direction is the net force?

  • Correct Answer: C) There is no net force.

Clicker Question 5 (Tension in a Pulley System)

  • Question: What is the tension in the string for this system of pulleys?

  • Answer: The correct answer is C) 12mg\frac{1}{2}mg

Class Problem: Books on a Table (Part 2)

  • Problem: Three books are stacked on a table (A, B, and C with masses 0.5 kg, 1 kg, and 2 kg respectively).

  • Task: Find the magnitude of all forces.

  • Solution:

    • Fg,EonA=4.9N\vec{F}_{g, E \, on \, A} = 4.9 \, N

    • Fg,EonB=9.8N\vec{F}_{g, E \, on \, B} = 9.8 \, N

    • Fg,EonC=19.6N\vec{F}_{g, E \, on \, C} = 19.6 \, N

    • FN,BonA=4.9N\vec{F}_{N, B \, on \, A} = 4.9 \, N

    • FN,AonB=4.9N\vec{F}_{N, A \, on \, B} = 4.9 \, N

    • FN,ConB=14.7N\vec{F}_{N, C \, on \, B} = 14.7 \, N

    • FN,BonC=14.7N\vec{F}_{N, B \, on \, C} = 14.7 \, N

    • FN,TonC=34.3N\vec{F}_{N, T \, on \, C} = 34.3 \, N

  • Labels: Book A, Book B, and Book C.

Newton’s 1st Law in Two Dimensions

  • Key Principle: Newton’s 1st Law works separately along each axis.

  • Example: Projectile Motion

    • No horizontal forces, so Fx=0\sum F_x = 0

    • No horizontal acceleration, so ax=0\, a_x = 0

  • Equations:

    • F<em>x,onA=0 if and only if a</em>A,x=0\sum F<em>{x, on \, A} = 0 \text{ if and only if } a</em>{A, x} = 0

    • F<em>y,onA=0 if and only if a</em>A,y=0\sum F<em>{y, on \, A} = 0 \text{ if and only if } a</em>{A, y} = 0

Clicker Question 6 (Sling Throws a Stone)

*Scenario: A sling throws a stone by releasing it as it swings in a circle.
*Question: What path would the stone take after release?
*Answer: A)

Lab 5: Net Force (Parts 2 and 3)

Newton’s 1st Law: Problem Solving Steps

  1. Diagram Situation

  2. Identify Objects of Interest

    • Know or want to know forces or acceleration.

  3. Identify Forces on Objects of Interest

  4. Freebody Diagram of Objects of Interest

    • Label objects.

    • Label type of force, “by” object and “on” object.

    • Ensure all “on” objects match diagram object.

    • Example: Person

      • Fg,byEonP\, \vec{F}_{g, by \, E \, on \, P} (Gravitational force)

      • FN,byGonP\, \vec{F}_{N, by \, G \, on \, P} (Normal force)

Newton’s 1st Law: Problem Solving Steps (Continued)

  1. Set up Newton’s 1st Law equation for each object of interest

    • General form: FonP=0\, \sum \vec{F}_{on \, P} = 0

    • Expand sum: F<em>g,byEonP+F</em>N,bygroundonP=0\, \vec{F}<em>{g, by \, E \, on \, P} + \vec{F}</em>{N, by \, ground \, on \, P} = 0

    • Write component equations:

      • F<em>g,x+F</em>N,x=0\, F<em>{g,x} + F</em>{N,x} = 0

      • F<em>g,y+F</em>N,y=0\, F<em>{g,y} + F</em>{N,y} = 0

    • Find components of each force:

      • F<em>g,x=0,F</em>g,y=mPg\, F<em>{g,x} = 0, F</em>{g,y} = -m_Pg

      • F<em>N,x=0,F</em>N,y=FN\, F<em>{N,x} = 0, F</em>{N,y} = F_N

    • Plug in each component:

      • m<em>Pg+F</em>N=0\,-m<em>Pg + F</em>N = 0

      • 0+0=0\, 0 + 0 = 0

  2. Solve for variables of interest

    • F<em>N=m</em>Pg\, F<em>N = m</em>Pg

Problem Solving Suggestions

  1. Acceleration is often implied (a=0\vec{a} = 0 for constant velocity)

  2. Tension points in the direction of ropes/string/etc.

    • Same angles on forces as angles in situation.

    • Find angle of rope means find direction of tension force.

  3. Negligible mass (“very light”, “massless”, …)

    • Ignore weight: Fg0\, \vec{F}_g \sim 0

    • Tension constant magnitude throughout “string”.

  4. Rotate axes to align with the majority of forces (especially on tilted surface)

General Physics I Fall 2023 Quiz 2 (Version B): Question 1 Walkthrough

  • Problem: A 20 kg block is dragged up the ramp at a constant speed with a rope. The coefficient of kinetic friction between the ramp and block is 0.5. What is the tension in the rope?

  • Solution Steps:

    • Draw a Free Body Diagram (FBD).

    • List knowns: Mass m=20kg\, m = 20 \, kg, coefficient of friction μk=0.5\, \mu_k = 0.5, and acceleration a=0\, a = 0.

    • Identify forces:

      • Tension force FT\, F_T

      • Normal force FN\, F_N

      • Weight W=mg\, W = mg

      • Kinetic Friction F<em>k=μ</em>kFN\, F<em>k = \mu</em>k F_N

    • Establish coordinate system where x is parallel to the ramp and y is perpendicular.

    • Express components of Weight W\, W:

      • Parallel: mgsin(θ)\, mg\sin(\theta)

      • Perpendicular: mgcos(θ)\, mg\cos(\theta)

    • Since a=0\, a=0, F=0\, \sum F = 0

    • Fx=0\, \sum F_x = 0

    • Fy=0\, \sum F_y = 0

    • F<em>Tx+F</em>kx+Wx=0\, \sum \vec{F}<em>{Tx} + \vec{F}</em>{kx} + \vec{W_x} = 0

    • F<em>Ty+F</em>Ny+Wy=0\, \sum \vec{F}<em>{Ty} + \vec{F}</em>{Ny} + \vec{W_y} = 0

    • Find Tension, FT=(0.5m˙gcos(θ))+mgsin(θ)\, F_T = (0.5 \dot mg \cos(\theta)) + mg \sin(\theta)

    • =mg(μkcos˙(θ)+sin(θ))\, = mg(\mu_k \dot \cos(\theta) + \sin(\theta))

General Physics I Fall 2023 Quiz 2 (Version B): Question 2 Walkthrough

  • Problem: A spring hangs vertically with no weight on it and no tension in it. In this state, it has a length of 10 cm. Then a 200 g weight is attached to the bottom, which stretches it until it is 25 cm long. Find the spring constant of the spring.

  • Solution Steps:

    • Apply equilibrium of forces.

    • F=0\sum F = 0

    • Free body force diagram. There is a gravitational force going down and Tension going up.

    • F<em>igy+F</em>ty=0\sum F<em>{igy} + F</em>{ty}=0

    • mg+k(Δx)=0-mg + k(\Delta x) = 0

    • Rearrange to solve for k

    • \k = \frac{mg}{(\Delta x)}

General Physics I Fall 2023 Quiz 2 (Version B): 3 Conceptual Multiple-Choice Questions.

  • 1. A stationary block rests on a ramp as a rope pulls it to the right. Which free body diagram matches the situation?

  • 2. A pendulum is swinging back and forth, as shown in the figure to the right. At which point is the tension the smallest?

  • 3. Which of the following pairs of forces are always equally large but in opposite directions, regardless of the motion of the objects?

Extra Credit Essay (Worth up to 10pts)

  • A) State one of Newton’s Laws in words, using the “better phrasing” discussed in class or equivalently accurate wording.

  • B) State another of Newton's Laws in words, using the “better phrasing” discussed in class or equivalently accurate wording.

  • C) State the last Newton’s Laws in words, using the “better phrasing” discussed in class or equivalently accurate wording.

  • D) Identify which of the three answers above are Newton’s 1st Law, Newton’s 2nd Law, and Newton’s 3rd Law.

Example Problem: Slippery Slope

  • Problem Statement: A woman walks up a slick slope at a steady pace, trying not to slip down. If the coefficient of static friction between her shoes and the ground is 0.5, what is the steepest slope she can climb?

  • Answer: 26.6 degrees off the horizontal.

  • Key Concepts:

    • Static Friction: The force that prevents an object from starting to move.

    • Equilibrium: The state where the net force on an object is zero.

    • Free Body Diagram: A diagram showing all forces acting on an object.

    • Components of Forces: Breaking forces into horizontal and vertical components for easier analysis.

  • Solution Approach:

    • Draw a Free Body Diagram (FBD).

      • Forces on the person:

        • Gravitational force Fg\, F_g

        • Normal force FN\, F_N

        • Static friction force Fs\, F_s

    • Set up coordinate system where y is parallel to the ramp and x is perpendicular.

    • Relate the angle to the coefficient of static friction.

Clicker Question 7 (Stationary Box)

  • Which FBD best illustrates forces on Stationary Box?

  • Correct Answer: D

Clicker Question 8 (Angles in Box FBD)

  • Question: Which angle(s) in the box FBD are equal to θ\, \theta in the figure?

  • Correct Answer: (A)

Clicker Question 9 (Stationary Ramp)

  • Question: Which FBD best illustrates the forces on the stationary ramp?

  • Correct Answer: A

Clicker Question 10 (Angles in Ramp FBD)

*Question: Which angle(s) in the ramp FBD are equal to θ\, \theta in the figure?
*Correct Answer: B

Clicker Question 11 (Newton's 3rd Law Pairs)

*Question: Which pairs of forces are Newton's 3rd Law pairs?
*Correct Answer: D)

Class Problem: Box & Ramp Forces

  • Problem Statement: Find the magnitude of each forces on both the box and ramp, both of which remain stationary.

  • Provided Information:

    • Box stationary

    • Ramp stationary

    • Angle θ=30\, \theta = 30

  • Break Down:

    • A == Adjacent.

    • O == Opposite

  • Therefore Pythagorean theory is required

  • FS,,y=m<em>g</em>cos(0)F_{S,,y}=-\,m<em>g</em>cos(0)

Net Force & Acceleration: Newton's 2nd Law

Causing Motion Discussion

  • Discussion Points:

    • What causes motion?

      • Net force causes acceleration.

      • Acceleration leads to speeding up, slowing down, or turning.

Mistaken Intuition on Forces

  • Intuition: Forces cause velocity.

    • Velocity is in direction of force.

    • Without net force, objects stop.

    • vF\, \vec{v} \propto \vec{F}

  • Reality: Forces cause acceleration.

    • Acceleration is in the direction of force.

    • Without net force, velocity doesn’t change.

    • aF\, \vec{a} \propto \vec{F}

  • Apparent vs Actual Situations

    • Apparent situation: Net force at constant velocity.

    • Actual situation: No net force at constant velocity.

  • Friction: Friction is the reason that most objects require an applied force to move along the ground.

Newton's Second Law

  • Basic Idea: Net force produces acceleration.

  • Generalizes Newton’s First Law

  • Equation: F<em>onA=m</em>AaA\, \sum \vec{F}<em>{on \, A} = m</em>A \vec{a}_A

  • Where:

    • FonA\, \sum \vec{F}_{on \, A} is the net force on generic object “A.”

    • mA\, m_A is the mass of “A.”

    • aA\, \vec{a}_A is the acceleration of “A.”

  • F\, \sum \vec{F} & a\, \vec{a} point in same direction!

Clicker Question 12 Braking Car

*Question: A car brakes to a stop. While braking, which direction is the net force on the car?
*Correct Answer: A
*The net force direction is toward the rear of the car.

Clicker Question 13 Braking Car Passenger

*Question: A car brakes to a stop. While braking, which direction is the net force on the passenger?
*Correct Answer: A
*The New Force Direction: Towards The rear of car

Clicker Question 14 Braking Car Forces

*Question: A car brakes to a stop. While braking, which experiences the largest net force?
*Correct Answer: B
*The car experiences the largest net force

Newton’s 2nd Law: Problem Solving Steps

  1. Diagram situation

  2. Identify objects of interest

    • Know or want to know forces or acceleration

  3. Identify forces on objects of interest

  4. Freebody diagram objects of interest

    • Label objects

    • Label type of force, “by” object and “on” object

    • Make sure all “on” objects match diagram object

    • [Person (jumping)]

      • Gravitational force, Fg,byEonP\, \vec{F}_{g,by \, E \, on \, P}

      • Normal force, FN,byGonP\, \vec{F}_{N,by \, G \, on \, P}

Newton’s 2nd Law: Problem Solving Steps

  1. Set up Newton’s 2nd Law equation for each object of interest

    • General form: F<em>onP=m</em>PaP\, \sum \vec{F}<em>{on \, P} = m</em>Pa_P

    • Expand sum: F<em>g,byEonP+F</em>N,bygroundonP=m<em>Pa</em>P\, \vec{F}<em>{g,by \, E \, on \, P} + \vec{F}</em>{N,by \, ground \, on \, P} = m<em>Pa</em>P

    • Write component equations: F<em>g,x+F</em>N,x=m<em>Pa</em>P,y,F<em>g,y+F</em>N,y=m<em>Pa</em>P,x\, F<em>{g,x} + F</em>{N,x} = m<em>Pa</em>{P,y}, F<em>{g,y} + F</em>{N,y} = m<em>Pa</em>{P,x}

    • Find components of each force and acceleration:

      • F<em>g,x=0,F</em>g,y=m<em>Pg,F</em>N,x=0,F<em>N,y=F</em>N,a<em>P,x=0,a</em>P,y=a\, F<em>{g,x} = 0, F</em>{g,y} = -m<em>Pg, F</em>{N,x} = 0, F<em>{N,y} = F</em>N, a<em>{P,x} = 0, a</em>{P,y} = a

    • Plug in each component:m<em>Pg+F</em>N=mPa,0+0=0\,-m<em>Pg + F</em>N = m_Pa, 0 + 0 = 0

  2. Solve for variables of interest (F<em>N=m</em>P(g+a))\, (F<em>N = m</em>P(g + a))

Problem Solving Suggestions

  1. Acceleration is often implied (a=0\vec{a} = 0 for constant velocity)

  2. Tension points in the direction of ropes/string/etc.

    • Same angles on forces as angles in situation.

    • Find angle of rope means find direction of tension force.

  3. Negligible mass (“very light”, “massless”, …)

    • Ignore weight Fg0\, \vec{F}_g \sim 0, approximately zero net force ma0\, ma \sim 0

    • Tension constant magnitude throughout “string”

  4. Rotate axes to align with majority of forces (esp. on tilted surface)

New steps in bold

Freefall Revisited

  • Revised definition

    • An object is in freefall if only gravitational forces act on it

  • Why does a=g\, a = g in freefall?

    • Newton’s 2nd Law explanation

      • Step 1: F<em>onA=m</em>AaA\, \sum \vec{F}<em>{on \, A} = m</em>A\vec{a}_A

      • Step 2: F<em>g,EarthonA=m</em>AaA\, \vec{F}<em>{g,Earth \, on \, A} = m</em>A\vec{a}_A

      • Step 3: m<em>Ag</em>Earth=m<em>Aa</em>A\, m<em>Ag</em>{Earth} = m<em>A\vec{a}</em>A

      • Step 4: g<em>Earth=a</em>A\, g<em>{Earth} = \vec{a}</em>A

Finer Point: Which Acceleration to Use?

  • Basic issue

    • Newton’s Laws describes motion with one acceleration per object

    • …but which acceleration?

  • Currently limited to objects that only have one acceleration

    • Point particles

      • Negligible dimensions so only one position

    • Rigid, non-rotating objects

      • All pieces share the same acceleration

  • Later we will define which acceleration it describes for any object

Class Problem: Books in an Elevator

The table from the previous problem is placed in an elevator accelerating at 1 m/s^2 upward. What are all the forces now?

  • Fg,E=4.9N\, F_{g,E} = 4.9N

  • Fg,E=9.8N\, F_{g,E} = 9.8N

  • Fg,E=19.6N\, F_{g,E} = 19.6N

Lab 6: Unbalanced Forces

Newton's Laws Recap

Forces & Motion:
  • 1st:

    F<em>onA=0iffa</em>A=0\, \sum \vec{F}<em>{on A} = 0 iff \vec{a}</em>A = 0

  • 2nd:

    F<em>onA=m</em>AaA\, \sum \vec{F}<em>{on A} = m</em>A*\vec{a}_A

Forces as interaction:
  • 3rd:

    F<em>byAonB=F</em>byBonA\,\vec{F}<em>{by A on B} = - \vec{F}</em>{by B on A}

Class Problem: Slipping Down

A box of unknown mass is set on a board, as shown. The board is tilted up until the box begins to slip. If the coefficient of friction is 0.6 (static) and 0.4 (kinetic) between the board and box, find:

  • The angle at which the box begins to slip. 31.0°

  • The speed it reaches right before hitting the floor. 0.71 m/s

Example Problem:

Atwood Machine

What's the acceleration of the masses?

Class Problem: A Balanced Design

al blocks remain stationary, if the weight of the rope and frictional forces are both negligible?
an the blocks remain stationary: Answer = 𝟏𝟗. 𝟓°