Resource Lesson
Static Equilibrium
Printer Friendly Version
When forces acting on an object which is at rest are balanced, then we say that the object is in a state of
static equilibrium
.
The resultant of these forces equals zero. That is, the vector sum of the forces adds to zero.
Example #1
Suppose two dogs are struggling for the same shoe as shown in the diagram below.
The left dog's force is shown by the yellow/black arrow while the right dog's force is shown by the teal arrow. Notice below that when the forces are added headtotail, the resultant force, shown in grey, acts straight up the yaxis.
Force
_{right dog}
+ Force
_{left dog}
= Resultant
F
_{r}
+
F
_{l}
=
R
To place the shoe into a state of static equilibrium, a third force (shown in red) would have to be added to the diagram. Then the forces exerted on the shoe would equal zero.
Force
_{right dog}
+ Force
_{left dog}
+ "Equilibrium" vector = 0
F
_{r}
+
F
_{l}
+
E
= 0
F
_{r}
+
F
_{l}
=
E
By comparing the vector equations presented above
F
_{r}
+
F
_{l}
=
R
F
_{r}
+
F
_{l}
=
E
we notice that the
third force required for equilibrium to be established is a vector that has the same magnitude as the resultant, but points in 180º the opposite direction
.
R = E
Each dog's force has been resolved into its x and ycomponents.
A vector diagram showing only the components of each dog's force.
The addition of a third force would place the shoe into a state of static equilibrium.
Example #2
Suppose you are asked to calculate the tensions in the three ropes (
A
,
B
,
C
) that are supporting the 5kg mass shown below. Since the system is at rest, we will work the problem using the properties of static equilibrium.
Let's begin with a
freebody diagram showing the forces acting on the knot
. Since these forces belong to three separate ropes, all three tensions can be different.
The next step will be to build an
xy
chart showing the components of each force.
If θ were to equal 37º then
Since we do not have any knowledge of any of the three tensions, we must now do a similar analysis using a
freebody diagram of the 5kg mass
.
The
xy
chart for the 5kg mass would look as follows:
Since we know that the 5kg mass is in static equilibrium, we know that the sum of the forces in each column equals zero. We only need to write the equation for the ycolumn since there are no nonzero forces in the xcolumn.
y:
C
+ (mg) = 0
C
 5(9.8) = 0
C
= 49 N
Now, knowing the value for
C
, we can solve for the tensions in ropes
A
and
B
by setting up the following equations from each column in our
xy
chart for the knot:
x:

A
cos(37º) +
B
= 0
y:
A
sin(37º) 
C
= 0
x:
0.8
A
+
B
= 0
y:
0.6
A

C
= 0
Since we know the value for
C
we will next solve for
A
and then for
B
.
y:
0.6
A
 49 = 0
A
= 49/0.6
A
= 81.7 N
x:
0.8(81.7) +
B
= 0
B
= 0.8(81.7)
B
= 65.3 N
Example #3
This procedure can also be applied to the following situation in which a mother is just at the instant of releasing her child in a swing.
Refer to the following information for the next four questions.
Suppose the child in the illustration above has a mass of 15 kg and the angle the swing makes with the horizontal is 75º. See if you can model the example with the 5kg mass and answer each of these questions.
How much does the child weigh?
What is the total tension required in all four "chains"?
How large a restraining force does the parent supply?
If four chains are actually supporting the swing, what is the tension in each individual chain?
In cases where the rope passes over a massless, frictionless pulley the tension on either side of the pulley is the same. This term really means that we are not considering the pulley to have any rotational inertia; that is, the rope slides over the pulley without causing it to rotate. When pulleys with rotational inertia are used, we have to assign different tensions to the ropes on each side and calculate the torque produced on the pulley.
Example #4
Consider this next system in which both suspended blocks have a mass of 1.5 kg and the pulley has a mass of 1.0 kg.
Since all of the forces are vertical, we can easily identify the tensions in each of the three ropes by setting the "sum of the magnitudes of the downward forces" equal to the "sum of the magnitudes of the upward forces."
Isolating each block and then the pulley we can generate the following freebody diagrams and their equations.
T
_{2}
= m
g
T
_{3}
= m
g
T
_{1}
=
T
_{2}
+ m
g
+
T
_{3}
T
_{2}
= (1.5)(9.8)
T
_{2}
= 14.7 N
T
_{3}
= (1.5)(9.8)
T
_{3}
= 14.7 N
T
_{1}
= 14.7 + 1(9.8) + 14.7
T
_{1}
= 39.2 N
If the masses had been unequal, then the system would have
accelerated in the direction of the greater mass
. Yet, even during that period of acceleration, the tensions
T
_{2}
and
T
_{3}
would have remained equal.
Summary Example
Let's use all of the properties learned on this page to now determine the mass of the monkey. In the process, also calculate
T
_{1}
,
T
_{2}
,
T
_{3}
,
T
_{4}
,
T
_{5}
,
T
_{6}
, and
W
_{2}
if
W
_{1}
equals 350 N. If you need assistance getting started, reference the information in the hints located to the left of each question.
left knot
T
_{1}
T
_{3}
T
_{4}
right knot
T
_{5}
T
_{2}
W
_{2}
pulley
T
_{6}
mass
_{monkey}
Related Documents
Lab:
Labs 
Coefficient of Friction
Labs 
Coefficient of Friction
Labs 
Coefficient of Kinetic Friction (pulley, incline, block)
Labs 
Conservation of Momentum in TwoDimensions
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 
LooptheLoop
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 ReBounding 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 
Nonconstant Resistance Forces
RL 
Properties of Friction
RL 
Springs and Blocks
RL 
Springs: Hooke's Law
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 
ActionReaction #1
CP 
ActionReaction #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 
Headon Collisions #1
NT 
Headon 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 
Twoblock 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 
Distinguishing 2nd and 3rd Law Forces
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 © 19972021
Catharine H. Colwell
All rights reserved.
Application Programmer
Mark Acton