Worksheet
Distinguishing 2nd and 3rd Law Forces
Printer Friendly Version
Your weight is the result of the gravitational force of the earth on your body. Describe the corresponding reaction force.
If you step off a ledge, you accelerate noticeably toward the earth because of the gravitational interaction between you and the earth. Does the earth accelerate towards you as well? Explain
When a high jumper leaves the ground, what is the source of the upward force that accelerates her? What force acts on her once her feet are no longer in contact with the ground?
Refer to the following information for the next two questions.
A bicycle and a massive truck have a head-on collision.
Upon which vehicle is the impact force greater?
bicycle
truck
Which vehicle undergoes the greater change in its motion?
bicycle
truck
Refer to the following information for the next two questions.
A speeding bus makes contact with a lovebug that splatters onto its windshield. Because of the sudden impact force, the unfortunate bug undergoes a sudden loss of speed.
Is the corresponding impact force that the bug exerts against the windshield of the bus greater, the same, or less than that which it experienced?
greater than
the same
less than
Is the resulting change in speed of the bus greater than, the same, or less than that of the bug?
greater than
the same
less than
Refer to the following information for the next three questions.
Suppose you exert 200-N of force on your refrigerator and push it across the kitchen floor at a constant velocity.
How large is the friction force that acts between the refrigerator and the floor?
Does the friction force cancel your applied 200 N-force, thus making acceleration impossible?
yes
no
Could the friction force be defined as the reaction force to your applied force?
yes
no
Refer to the following information for the next question.
Since the force that acts on a bullet when a gun is fired is equal and opposite to the force that acts on the gun, does this imply a zero net force and therefore the impossibility of an accelerating bullet? Explain.
Refer to the following information for the next three questions.
Consider the two forces acting on the person who stands still, namely the downward pull of gravity, mg, and the upward support of the floor,
.
Are these forces equal and opposite?
yes
no
Do they form an action-reaction pair? That is, are they 3rd Law forces?
yes
no
Do they cancel each other making acceleration equal to zero? That is, are they 2nd Law forces?
yes
no
Refer to the following information for the next three questions.
Two 100 N weights are attached to a spring scale as shown.
Does the spring scale read 0 N, 100 N, or 200 N?
0 N
100 N
200 N
Would the spring scale reading change if the left pulley was removed and the left string attached to a stationary vertical pole?
While the left string is attached to a stationary vertical pole, the left 100 N weight is suspended underneath the original right-hand 100 N weight.
Does the spring scale read 0 N, 100 N, or 200 N?
0 N
100 N
200 N
Refer to the following information for the next three questions.
An athlete holds a barbell stationary overhead.
How does the force he must exert compare to the weight of the barbell?
less than
the same
greater than
When the barbell was being accelerated upward, how did the athlete's applied force compare to the weight of the barbell?
less than
equal to
greater than
When the barbell is being accelerated downward, how does the athlete's applied force compare to the weight of the barbell?
less than
the same
greater than
Refer to the following information for the next two questions.
Suppose two carts, one twice as massive as the other, fly apart when the compressed spring that joins them is released.
How does the force exerted by the spring on the 1m-cart compare to the force exerted by the spring on the 2m-cart?
less than
equal to
greater than
How fast does the 2m-cart roll compared to the smaller 1m-cart?
Refer to the following information for the next four questions.
Consider the following 100-N hanging weight.
The tension in the string could be called F
SM
, that is, the force of the
string on the mass
.
The mass' weight could be called F
EM
, that is, the force of the
earth on the mass
.
Are these two forces, F
SM
and F
EM
, 2nd Law forces or 3rd Law forces?
2nd Law forces
3rd Law forces
Can these forces cancel each other? Why or why not?
What is the reaction force for F
SM
?
The magnitudes of the forces F
SM
and F
MS
are equal and act in opposite directions. Can they cancel each other?
yes
no
Related Documents
Lab:
Labs -
Coefficient of Friction
Labs -
Coefficient of Friction
Labs -
Coefficient of Kinetic Friction (pulley, incline, block)
Labs -
Conservation of Momentum in Two-Dimensions
Labs -
Falling Coffee Filters
Labs -
Force Table - Force Vectors in Equilibrium
Labs -
Inelastic Collision - Velocity of a Softball
Labs -
Inertial Mass
Labs -
LabPro: Newton's 2nd Law
Labs -
Loop-the-Loop
Labs -
Mass of a Rolling Cart
Labs -
Moment of Inertia of a Bicycle Wheel
Labs -
Relationship Between Tension in a String and Wave Speed
Labs -
Relationship Between Tension in a String and Wave Speed Along the String
Labs -
Static Equilibrium Lab
Labs -
Static Springs: Hooke's Law
Labs -
Static Springs: Hooke's Law
Labs -
Static Springs: LabPro Data for Hooke's Law
Labs -
Terminal Velocity
Labs -
Video LAB: A Gravitron
Labs -
Video LAB: Ball Re-Bounding From a Wall
Labs -
Video Lab: Falling Coffee Filters
Resource Lesson:
RL -
Advanced Gravitational Forces
RL -
Air Resistance
RL -
Air Resistance: Terminal Velocity
RL -
Forces Acting at an Angle
RL -
Freebody Diagrams
RL -
Gravitational Energy Wells
RL -
Inclined Planes
RL -
Inertial vs Gravitational Mass
RL -
Newton's Laws of Motion
RL -
Non-constant Resistance Forces
RL -
Properties of Friction
RL -
Springs and Blocks
RL -
Springs: Hooke's Law
RL -
Static Equilibrium
RL -
Systems of Bodies
RL -
Tension Cases: Four Special Situations
RL -
The Law of Universal Gravitation
RL -
Universal Gravitation and Satellites
RL -
Universal Gravitation and Weight
RL -
What is Mass?
RL -
Work and Energy
Worksheet:
APP -
Big Fist
APP -
Family Reunion
APP -
The Antelope
APP -
The Box Seat
APP -
The Jogger
CP -
Action-Reaction #1
CP -
Action-Reaction #2
CP -
Equilibrium on an Inclined Plane
CP -
Falling and Air Resistance
CP -
Force and Acceleration
CP -
Force and Weight
CP -
Force Vectors and the Parallelogram Rule
CP -
Freebody Diagrams
CP -
Gravitational Interactions
CP -
Incline Places: Force Vector Resultants
CP -
Incline Planes - Force Vector Components
CP -
Inertia
CP -
Mobiles: Rotational Equilibrium
CP -
Net Force
CP -
Newton's Law of Motion: Friction
CP -
Static Equilibrium
CP -
Tensions and Equilibrium
NT -
Acceleration
NT -
Air Resistance #1
NT -
An Apple on a Table
NT -
Apex #1
NT -
Apex #2
NT -
Falling Rock
NT -
Falling Spheres
NT -
Friction
NT -
Frictionless Pulley
NT -
Gravitation #1
NT -
Head-on Collisions #1
NT -
Head-on Collisions #2
NT -
Ice Boat
NT -
Rotating Disk
NT -
Sailboats #1
NT -
Sailboats #2
NT -
Scale Reading
NT -
Settling
NT -
Skidding Distances
NT -
Spiral Tube
NT -
Tensile Strength
NT -
Terminal Velocity
NT -
Tug of War #1
NT -
Tug of War #2
NT -
Two-block Systems
WS -
Advanced Properties of Freely Falling Bodies #1
WS -
Advanced Properties of Freely Falling Bodies #2
WS -
Calculating Force Components
WS -
Charged Projectiles in Uniform Electric Fields
WS -
Combining Kinematics and Dynamics
WS -
Force vs Displacement Graphs
WS -
Freebody Diagrams #1
WS -
Freebody Diagrams #2
WS -
Freebody Diagrams #3
WS -
Freebody Diagrams #4
WS -
Introduction to Springs
WS -
Kinematics Along With Work/Energy
WS -
Lab Discussion: Gravitational Field Strength and the Acceleration Due to Gravity
WS -
Lab Discussion: Inertial and Gravitational Mass
WS -
net F = ma
WS -
Practice: Vertical Circular Motion
WS -
Ropes and Pulleys in Static Equilibrium
WS -
Standard Model: Particles and Forces
WS -
Static Springs: The Basics
WS -
Vocabulary for Newton's Laws
WS -
Work and Energy Practice: Forces at Angles
TB -
Systems of Bodies (including pulleys)
TB -
Work, Power, Kinetic Energy
PhysicsLAB
Copyright © 1997-2025
Catharine H. Colwell
All rights reserved.
Application Programmer
Mark Acton