Chapter 2 Interactions: Forces · Lesson 3
Resolving Forces & Free-Body Analysis
Applications of force resolution · Free-body analysis and equilibrium of concurrent forces
PhyLab · Physics Lessons
Review of last lesson
Changing Friction · Combining Forces
Sudden changes in friction
Static→Static
Push changes, object stays put: static friction adjusts its size or direction
Static→Kinetic
Push exceeds max static friction: object slides, friction turns kinetic
Kinetic→Static
Object slows to rest: friction turns static, sized by equilibrium
Kinetic→Kinetic
Relative motion reverses (e.g. a belt jams): kinetic friction flips
Critical point
Max static friction = onset of sliding; on belts, equal speeds is the switch
Composing & resolving forces
Concurrent
Forces at one point, or whose lines of action meet at one point
Resultant
An equivalent replacement, not an extra force; may be larger or smaller than a part
Rules
Parallelogram rule: diagonal = resultant; triangle rule: head to tail
Resolution
Inverse of composition: by actual effect, or into x–y components
Vectors
Vectors add by the parallelogram rule; scalars by arithmetic
Example 1 · Resolving by effect
Carpenters often drive a wedge in to lock a tenon joint. The right-triangle wedge shown has a base of 35 mm and a height of 5 mm. When it is driven in by a horizontal force F, the pressing force exerted by its slanted face is about (  )
Diagram of a wedge being driven into a tenon joint
A. 7F
B. 7.07F
C. 0.14F
D. 1.01F
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Answer B Resolve F perpendicular to the slanted face and perpendicular to the base. The force triangle is similar to the wedge triangle:
F to F2 equals h to L; L equals the square root of 35 squared plus 5 squared millimetres, about 35.4 mm; F2 equals L over h times F, about 7.07F
Practice 1 · Multiple answers
As shown, a downward force F of 180 N is resolved into two components F₁ and F₂. The angle between F₁ and F is α = 37°, and the angle between F₂ and F is θ. Given sin 37° = 0.6 and cos 37° = 0.8, which statements are correct? (  )
Diagram of force F resolved into F1 and F2
A. When θ = 90°, F₂ = 240 N
B. When θ = 37°, F₂ = 112.5 N
C. When θ = 53°, F₂ = 144 N
D. Whatever the value of θ, F₂ can never be less than 108 N
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Answer BD θ = 90°: F₂ = F tan 37° = 135 N; θ = 37°: F₁ = F₂ = 112.5 N; at θ = 53°, F₂ ⊥ F₁ and F₂ takes its minimum F sin 37° = 108 N
Model 1
Sliding Knots vs Fixed Knots
Sliding
Formed where a rope passes over a pulley or a smooth hook. It is really one rope: the tensions in the two segments are always equal, and their resultant lies along the angle bisector
A smooth hook hanging on a rope over a semicircular frame
Fixed
The rope on either side of the knot becomes two separate ropes, so the tensions in the two segments are not necessarily equal
A rope knotted at O, tied to A and B, holding a weight
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A smooth hanger on a clothesline: the two tensions are always equal, and the angle depends only on the pole spacing and the rope length
Model 2
Hinged Rods vs Fixed Rods
Hinged rod: one end on a pivot or hinge
The force from a light hinged rod always acts along the rod
Hinged light rod OA and rope AB together support weight G
Fixed rod: one end built in (into a wall or the ground)
The force is not necessarily along the rod; find it from the equilibrium condition or Newton's second law
Fixed rod BC built into a wall with a pulley at its end; a rope over the pulley holds weight M
Example 2 · Sliding and fixed knots
As shown, a spider hangs at rest from a water pipe by its silk. Threads OM and ON make angles α and β with the vertical (α > β). Let F₁ and F₂ be the tensions in OM and ON. Then (  )
A spider hanging from a water pipe by two threads OM and ON
A. The vertical component of F₁ is greater than that of F₂
B. The vertical component of F₁ equals that of F₂
C. The horizontal component of F₁ is greater than that of F₂
D. The horizontal component of F₁ equals that of F₂
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Answer D The threads meet in a fixed knot at O, so the two tensions need not be equal. At O, horizontally: F₁ sin α = F₂ sin β, so the horizontal components are equal; since α > β, F₁ has the smaller vertical component
Example 3 · Hinged and fixed rods
In figure (a), a light rope AD passes over a light pulley fixed to the right end of horizontal beam BC and holds a mass m₁, with ∠ACB = 30°. In figure (b), light rod HG is hinged to a vertical wall at one end and held by string EG at the other; EG makes 30° with the horizontal, and string GF hangs a mass m₂ from point G. With gravitational acceleration g, which statement is correct? (  )
A. In (a), the force from BC on the pulley is
m1 g over 2
B. In (b), the force on rod HG from the strings is
m2g
C. Tension ratio
F AC
:
F EG
=
1 to 1
D. Tension ratio
F AC
:
F EG
=
m1 to 2 m2
Figure (a): a pulley at the right end of beam BC holds m1; figure (b): hinged light rod HG held by string EG, with m2 hanging from G
Example 3 Solution
(a) Fixed rod + pulley (sliding knot)
(b) Hinged rod + fixed knot
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Answer D
F AC equals m1 g, F EG equals 2 m2 g, so F AC to F EG equals m1 to 2 m2
; force from BC on the pulley is m₁g; force on rod HG is
root 3 times m2 g
Practice 2
A small crane: A and B are smooth light pulleys, C is a motor, and a light inextensible rope links them to object P. Pulley A's axle rides on a horizontal telescopic arm; pulley B rides on a vertical one. With P at rest (  )
Small crane: pulley A on a horizontal arm, pulley B on top of a vertical arm, motor C at the base, object P hanging below A
A. The force on A's axle may be horizontal
B. The force on A's axle must exceed P's weight
C. Moving only A right increases the force on its axle
D. Moving only B up increases the force on A's axle
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Answer C A is a sliding knot: both rope segments carry tension G, and the axle force is their resultant. The angle θ lies between 90° and 180°, so the resultant cannot be horizontal and can be greater than, equal to, or less than G. Moving A right makes θ smaller and the resultant larger; moving B up makes θ larger and the resultant smaller
Chapter 2 Interactions: Forces
Part 2
Free-Body Analysis · Equilibrium of Concurrent Forces
Choose the object to study in a real situation, decide whether normal and friction forces act and in which direction, and use the equilibrium condition for concurrent forces to solve problems
Key ideas
1. Free-Body Analysis
The process of finding every force that acts on the chosen object in a given physical situation, and drawing a free-body diagram
The usual order
Step 1
Field forces
Gravity, electric and magnetic forces
Step 2
Contact forces
Normal forces and friction: check each contact surface in turn
Step 3
Other forces
Pulls, pushes and other forces given in the problem
Draw only real forces on the object: every force must have something that exerts it. A "sliding-down force" is just a component of gravity, so do not draw it as an extra force
Key ideas
2. Equilibrium of Concurrent Forces
1 Equilibrium
The object is at rest or in uniform straight-line motion, i.e. a = 0
2 Condition
Fnet = 0; equivalently, the net force in the x direction and in the y direction are each zero
3 Perpendicular components
Resolve every force along perpendicular x and y axes. Adding the x components gives Fₓ, adding the y components gives the net y force, and these combine into F
Choose axes so that as many forces as possible lie along them
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Project each force onto the axes → add components head to tail on each axis → combine
Key ideas
3. Consequences of Equilibrium
2 forces
The two forces must be equal in size and opposite in direction
3 forces
Any one force is equal and opposite to the resultant of the other two
Placed head to tail, the three forces close a triangle
n forces
Any one force is equal and opposite to the resultant of all the others
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From the textbook
A child slides down a slide inclined at θ at constant speed. If the angle θ is increased, do the forces on the child change? Can the child still slide down at constant speed?
A children's slide
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Hint At constant speed, kinetic friction equals the component of gravity along the slope. With a steeper slope: gravity mg is unchanged; the normal force mg cos θ decreases, so friction μmg cos θ decreases; the component along the slope mg sin θ increases ⇒ no longer constant speed: the child speeds up
Check 1 · True or false
A stone arch has a top made of six identical stones, as sketched. Stones 1 and 6 are fixed; stones 2 and 5 each have mass m; stones 3 and 4 each have mass m′. Friction between stones is negligible, and gravitational acceleration is g.
A semicircular stone arch made of six stones numbered 1 to 6
(1) Stones 2, 3, 4 and 5 are each in equilibrium under three forces
(2) The normal force between stones 3 and 4 is zero
(3) The normal force of stone 1 on stone 2 equals (m + m′)g
(4) An object in equilibrium must have zero acceleration
True Each stone feels only gravity and the normal forces from its two contact faces
False The 3–4 contact face is vertical; without a normal force there, stone 3 could not balance
False Treating 2 and 3 as one system, only the vertical component of the force from 1 on 2 equals (m + m′)g
True Equilibrium means zero net force, so a = 0
Check 2
As shown, a football in a net bag hangs from point A
on a smooth wall, touching it at B. Its weight is G; rope AC
makes angle α with the wall. Wall force: F
N
; tension: F
T
.
Ignore the weight of the net. Which relation is correct? (  )
A football in a net bag hung from point A on a smooth wall, touching the wall at B
A. F
T
 = F
N
B. F
T
 < F
N
C. F
T
 > G
D. F
T
 < G
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Answer C Gravity, the wall's normal force and the rope tension balance. Head to tail they form a right triangle with the tension as the hypotenuse: tension = G/cos α > G
Check 3
A 2 kg shot is placed on a 45° incline and held by a vertical board, so it is at rest. Ignore friction on the shot and take g = 10 m/s². Then (  )
A shot on a 45° incline held by a vertical board
A. The shot feels 4 forces: gravity, the normal force from the incline, the normal force from the board, and a "sliding-down force"
B. The force from the board on the shot points up the incline
C. The force of the shot on the board is
10 root 2 newtons
D. The force of the shot on the incline is
20 root 2 newtons
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Answer D The shot feels only three forces: gravity G, the board's normal force F₁ (perpendicular to the board, horizontal to the right) and the incline's normal force F₂. A "sliding-down force" is a component of gravity, not an extra force
F1 equals G times tan 45 degrees equals 20 N; F2 equals G divided by cos 45 degrees equals 20 root 2 N
Topic 1 Free-body analysis
The picture shows a kitten leaping off the ground to chase a butterfly. Then (  )
A kitten leaping into the air after a butterfly
A. The flying butterfly is acted on by gravity only
B. When the butterfly turns, the net force on it is along its direction of motion
C. In the air, the kitten is acted on by gravity and a normal force
D. While pushing off, the normal force on the kitten is greater than its weight
A ✗ The butterfly is also pushed by the air
B ✗ On a curved path the net force points toward the inside of the curve, not along the motion
C ✗ In the air the kitten touches nothing, so there is no normal force
D ✓ Pushing off, the kitten accelerates upward from rest, so the ground's normal force exceeds its weight
Answer D
Topic 1 Free-body analysis
After cleaning the board, Ming sticks a magnetic eraser onto the vertical blackboard and sees it slowly slide down by itself. He moves it to another spot, where it stays still. Which statement is correct? (  )
A magnetic eraser stuck to a vertical blackboard
A. While slowly sliding down, the friction on the eraser is greater than its weight
B. While slowly sliding, the total force from the board on the eraser is vertically upward and equal to its weight
C. When at rest, the eraser feels only 3 forces
D. When at rest, the friction on the eraser is less than its weight
A ✗ Sliding slowly counts as constant speed, so it is in equilibrium and kinetic friction equals the weight
B ✓ The board's magnetic force, normal force and friction together balance gravity: vertically upward, equal to the weight
C ✗ At rest it feels 4 forces: gravity, magnetic force, normal force and static friction
D ✗ At rest, static friction balances gravity, so they are equal
Answer B
Key takeaway
Three Tests for Whether a Force Exists
Most basic
Conditions
Each kind of force needs its own conditions. First check whether the conditions for that force are met
e.g. a kitten in mid-air touches nothing, so no normal force
When conditions are unclear
Effects
Look at the object's state of motion, then use equilibrium or Newton's second law to find the unknown force
e.g. a resting eraser: friction must equal and oppose gravity
Forces come in pairs
Reaction
Forces are mutual: a force exists only if its reaction force exists
e.g. a "sliding-down force" has no source and no reaction, so it does not exist
Key takeaway
Steps for Free-Body Analysis
① Choose the object
It can be a single object or a group of objects
② Isolate it
Separate it from its surroundings and ask which nearby objects exert forces on it
③ Draw the diagram
Draw the free-body diagram and mark the direction of each force accurately
④ Check
Does every force have a source? Can these forces produce the state of motion given in the problem?
Topic 2 Applying the equilibrium condition
Methods for Static Equilibrium Problems
Method
How it works
Composition
Three concurrent forces in balance: the resultant of any two is equal and opposite to the third
Resolve by effect
Three concurrent forces in balance: resolve one force by its effects; each component balances one of the other two forces
Perpendicular components
Three or more forces in balance: resolve every force along two perpendicular directions; equilibrium holds in each direction
Force triangle
Three forces in balance: slide them head to tail into a closed vector triangle and solve with the sine rule, cosine rule or similar triangles
Example 1 · Composition and perpendicular components
A ball of mass m hangs from a vertical wall by string AB, which makes 60° with the wall. In figure (a), a pull F₁ at 120° to the string holds the ball at rest, and the string tension is Fa. In figure (b), a pull F₂ at 150° to the string holds the ball at rest, and the string tension is Fb. With gravitational acceleration g, which equation is correct? (  )
Figures (a) and (b): ball B hangs on string AB, pulled by F1 and F2 respectively
A.
F1 equals mg
B.
F2 equals 2mg
C.
F
a
equals root 3 times mg
D.
F
b
equals root 3 times mg
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Answer A Composition: the resultant of the pull and the string tension is equal and opposite to mg. In (a) the two forces are symmetric about the vertical, so F₁ and the tension both equal mg. In (b):
string tension
equals mg divided by cos 60 degrees equals 2mg; F2 equals mg times tan 60 degrees equals root 3 times mg
Summary
Solving Problems with the Equilibrium Condition
1
Choose the object
Pick something in equilibrium: a single object, a system, or even a knot
2
Draw the diagram
Analyse the forces on it and draw the free-body diagram
3
Compose or resolve
Three forces: compose or resolve directly Four or more: use perpendicular components
4
Write equations
Write equations from the equilibrium condition, solve, then discuss the result
Topic 3 Whole-system and isolation methods
Whole System vs Isolation
Whole system
Isolation
Idea
Treat several objects with the same acceleration as one body
Separate the chosen object from everything around it
Pros
Fewer forces, simpler calculation
Can find forces between objects inside the system
Cons
Cannot find forces between objects inside the system
More forces, more calculation
Use when
You need forces from outside the system, or the system's acceleration
You need forces between objects inside the system
Watch out
Do not draw internal forces between objects in the system
Usually isolate the object with fewer forces on it
The two methods are often combined: usually whole system first, then a part; if the forces on one object are already known, that part first, then the whole
Example 2 · Whole system and isolation
As shown, in one vertical plane, balls A and B are tied with inextensible strings a, b, c and d. The top of a hangs from a fixed vertical frame; d passes over the left fixed pulley and c over the right one, attached to identical counterweights P and Q. The pulley heights are adjusted until everything balances. Balls A, B and counterweights P, Q each have mass 50 g; strings c and d are parallel at θ = 30° to the horizontal (no friction). The tensions in a and b are (g = 10 m/s²) (  )
A. 2 N 1 N
B. 2 N 0.5 N
C. 1 N 1 N
D. 1 N 0.5 N
Balls A and B in a frame with strings a, b, c, d; pulleys on both sides hold counterweights P and Q
Example 2 Solution
Whole system for a, then isolate B for b
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Step 1 Whole system → tension in a
Treat A and B as one system: the tensions in c and d both equal the counterweight's weight mg, are parallel and opposite, and cancel. So the tension in a = 2mg = 1 N
Step 2 Isolate B → tension in b
B feels 2mg upward from a, its weight mg, a pull mg from d (down-left at 30°), and the tension in b. Horizontal part mg cos 30°, vertical part 0.5mg; combining, the tension in b = mg = 0.5 N
Answer D
Practice · Whole system and isolation
As shown, an incline of angle α is fixed on level ground. Two uniform balls P and Q sit between the incline and a fixed vertical board; P has twice the mass of Q. All surfaces are smooth and the system is at rest. If the line joining the centres of P and Q makes angle β with the vertical, which is correct? (  )
Balls P and Q between an incline and a vertical board; the line of centres makes angle β with the vertical
A. 4 tan α = tan β
B. 3 tan α = tan β
C. 2 tan α = tan β
D. tan α = tan β
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Answer B Let Q have mass m. Whole system: board force F₂ = 3mg tan α. Isolate Q: F₂ = mg tan β. Together: 3 tan α = tan β