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Belt Friction

Statics · FE Reference Handbook section

Statics
5 formulas
10 exam-style examples
~55 min
All Statics lectures

Learning objectives

What you must be able to do before leaving this section.

This chapter section covers Belt Friction within Statics. Read it the way you would read a textbook chapter: the theory first so the relations mean something, then every equation with its use and its trap, then 10 fully worked examples with the arithmetic shown line by line, and finally a self-check you should be able to answer without notes.

  • Explain, in your own words, what belt friction describes physically and when it applies.
  • State every one of the 5 relations the handbook lists here and name each symbol with its unit.
  • Select the correct relation from the wording of an exam stem within 20 seconds.
  • Carry a complete solution from givens to a "most nearly" answer with the correct unit.
  • Recognise the distractors generated by the unit trap: keep force in lbf or kN and distance in ft or m consistently.

Lecture

Why this section exists. Belt Friction is the part of Statics that lets you connect a determinate frame, truss or beam in equilibrium to a number you can defend. Before any equation is useful you must be able to picture the physical situation it describes; the schematic below is that picture.

How the theory is built. The handbook prints results, not derivations. Each relation in this section comes from one governing principle applied to the idealised system: state the principle, impose the stated assumptions, and the printed equation follows. Knowing which assumption each relation rests on is what lets you reject a wrong answer choice in seconds.

How it is examined. Items from this page are written as one free body, three equilibrium equations, one unknown reported. Roughly two thirds are direct substitution, one third require one intermediate quantity from a neighbouring relation, and a small number are conceptual — testing whether you know the assumption, not the arithmetic.

The habit that earns the points. Unit discipline. keep force in lbf or kN and distance in ft or m consistently. Every relation below is dimensionally consistent only when that rule is honoured, and the distractor set is deliberately built from candidates who ignored it. Write the unit next to every number you substitute, every time.

How to study this page. Read the theory, then cover the formula cards and try to reproduce each relation from its description. Then work the examples with the solution hidden, revealing one line at a time. Finish with the self-check questions; if you cannot answer one, return to the matching formula card.

Crane lowering a steel plate girder onto bridge bearings while ironworkers guide it.

Photo 1. Where this shows up in practice: belt friction.

Capstone Studio instructional photograph

BodyWNP

Statics — Belt Friction: reference schematic for orienting the symbols used in this section.

Theory, developed

Read this before the equations — it is what makes them memorable.

The physical situation

Every item from this section describes a determinate frame, truss or beam in equilibrium. Sketch it before you compute — a labelled sketch with the givens on it converts a wordy stem into a solvable problem and exposes the quantity the examiner left out on purpose.

The governing principle

The 5 relations on this page are consequences of one principle applied to that idealised system. Identify which quantity is conserved, balanced, or defined, and the correct equation follows without memorisation.

Assumptions and limits of validity

Each printed relation carries silent assumptions — linearity, steady state, uniformity, small deformation, or standard conditions, depending on the subject. Conceptual exam items are written by violating exactly one of these, so read the sentence above the equation as carefully as the equation itself.

Solution procedure you should automate

1) Read the last sentence of the stem to identify the requested quantity. 2) Locate the relation on this page whose left-hand side is that quantity. 3) Tabulate the givens with units and mark the missing symbol. 4) If a symbol is missing, find the one relation that produces it. 5) Rearrange symbolically, substitute once, evaluate, and round only at the end.

Crane lowering a steel plate girder onto bridge bearings while ironworkers guide it.

Photo 2. Statics: the physical system the theory above idealises.

Capstone Studio instructional photograph

Notation used in this section

F1Quantity produced by "F1 = F2 eµθ" — read its definition and unit from the handbook line directly above the equation.
F2Quantity produced by "F2 = force applied to resist impending motion" — read its definition and unit from the handbook line directly above the equation.
µQuantity produced by "µ = coefficient of static friction" — read its definition and unit from the handbook line directly above the equation.
θQuantity produced by "θ = total angle of contact between the surfaces expressed in radians" — read its definition and unit from the handbook line directly above the equation.

Handbook notes for this section

Definitions and conditions exactly as the handbook states them.

  • where

Core formulas for this FE topic

Definitions, applicability, units, assumptions and worked examples for each relation.

Worked exam-style examples

The four ways this section is written on the real exam — thoughts first, then equations, then substitution.

Example 1
Sliding of a construction crate

A 4.0 kN crate rests on a floor with μs = 0.35. What horizontal push starts it moving, and what push is needed on a 10° ramp (up-slope)?

Given

  • W = 4.0 kN
  • μs = 0.35
  • Ramp angle = 10°

Find

P on the level and P up the ramp

Start with the thinking

  • On the level, N equals the weight; on a ramp it does not.
  • Add the gravity component along the ramp.

Step-by-step solution

  1. Level friction — F = μs N = 0.35(4.0) = 1.40 kN

  2. Ramp normal

  3. Ramp friction

  4. Gravity component

  5. Required push

Answer: 1.40 kN level; 2.07 kN up the 10° ramp

Why the other options are there

  • 1.38 kN (gravity component omitted)
  • 2.09 kN (normal force taken as W on the ramp)

Reference: FE Reference Handbook — Statics — Friction

Example 2
Impending slip on an inclined plane — Belt Friction

A 569 lb crate rests on a 24° incline with μ_s = 0.55. Does it slip, and what force parallel to the incline is required to start it moving up?

Given

  • W = 569 lb
  • θ = 24°
  • μ_s = 0.55

Find

Slip check and required push

Start with the thinking

  • Compare the driving component to the maximum available friction.
  • Normal force uses the cosine, driving force the sine.
WWNP

Figure for Impending slip on an inclined plane — Belt Friction

Step-by-step solution

  1. Normal force — N = W·cos θ

  2. Substituting — N = 569·cos 24° = 519.8 lb

  3. Maximum friction — F_max = μ_s·N

  4. Substituting

  5. Driving component — W·sin θ = 569·sin 24° = 231.4 lb

  6. Compare — 231.4 < 285.9 → stays in place

  7. Push to move up — P = W·sin θ + μN = 517.3 lb

Answer: Stable; P ≈ 517.3 lb to move it up

Why the other options are there

  • 313.0 lb (weight used as the normal force)
  • -54 lb (friction sign reversed)

Reference: FE Reference Handbook — Statics → Belt Friction

Example 3
Torque to raise a load on a square screw thread — Belt Friction

A screw jack with a mean thread diameter of 1.50 in and a lead of 0.35 in per turn raises a 20,000 lb load. The coefficient of friction on the screw thread is 0.11. Find the required torque.

Given

  • W = 20,000 lb
  • d_m = 1.50 in
  • L = 0.35 in
  • μ = 0.11

Find

Torque required to raise the load

Start with the thinking

  • The screw thread is an inclined plane wrapped around a cylinder — the lead angle comes from the lead over the mean circumference.
  • Raising adds the friction angle to the lead angle; lowering subtracts it.

Step-by-step solution

  1. Formula

  2. Substituting

  3. Friction angle

  4. Formula

  5. Substituting

  6. Evaluate — T = 2,787 in·lb = 232.2 ft·lb

Answer: T ≈ 2,787 in·lb (232.2 ft·lb)

Why the other options are there

  • 1,114 in·lb (friction ignored)
  • 531.6 in·lb (lowering torque)

Reference: FE Reference Handbook — Statics → Belt Friction

Example 4
Impending slip on an inclined plane — Belt Friction (2)

A 691 lb crate rests on a 21° incline with μ_s = 0.40. Does it slip, and what force parallel to the incline is required to start it moving up?

Given

  • W = 691 lb
  • θ = 21°
  • μ_s = 0.40

Find

Slip check and required push

Start with the thinking

  • Compare the driving component to the maximum available friction.
  • Normal force uses the cosine, driving force the sine.
WWNP

Figure for Impending slip on an inclined plane — Belt Friction (2)

Step-by-step solution

  1. Normal force — N = W·cos θ

  2. Substituting — N = 691·cos 21° = 645.1 lb

  3. Maximum friction — F_max = μ_s·N

  4. Substituting

  5. Driving component — W·sin θ = 691·sin 21° = 247.6 lb

  6. Compare — 247.6 < 258.0 → stays in place

  7. Push to move up — P = W·sin θ + μN = 505.7 lb

Answer: Stable; P ≈ 505.7 lb to move it up

Why the other options are there

  • 276.4 lb (weight used as the normal force)
  • -10 lb (friction sign reversed)

Reference: FE Reference Handbook — Statics → Belt Friction

Example 5
Torque to raise a load on a square screw thread — Belt Friction (2)

A screw jack with a mean thread diameter of 1.00 in and a lead of 0.30 in per turn raises a 3,000 lb load. The coefficient of friction on the screw thread is 0.19. Find the required torque.

Given

  • W = 3,000 lb
  • d_m = 1.00 in
  • L = 0.30 in
  • μ = 0.19

Find

Torque required to raise the load

Start with the thinking

  • The screw thread is an inclined plane wrapped around a cylinder — the lead angle comes from the lead over the mean circumference.
  • Raising adds the friction angle to the lead angle; lowering subtracts it.

Step-by-step solution

  1. Formula

  2. Substituting

  3. Friction angle

  4. Formula

  5. Substituting

  6. Evaluate — T = 436.2 in·lb = 36.3 ft·lb

Answer: T ≈ 436.2 in·lb (36.3 ft·lb)

Why the other options are there

  • 143.2 in·lb (friction ignored)
  • 139.2 in·lb (lowering torque)

Reference: FE Reference Handbook — Statics → Belt Friction

Example 6
Impending slip on an inclined plane — Belt Friction (3)

A 834 lb crate rests on a 28° incline with μ_s = 0.25. Does it slip, and what force parallel to the incline is required to start it moving up?

Given

  • W = 834 lb
  • θ = 28°
  • μ_s = 0.25

Find

Slip check and required push

Start with the thinking

  • Compare the driving component to the maximum available friction.
  • Normal force uses the cosine, driving force the sine.
WWNP

Figure for Impending slip on an inclined plane — Belt Friction (3)

Step-by-step solution

  1. Normal force — N = W·cos θ

  2. Substituting — N = 834·cos 28° = 736.4 lb

  3. Maximum friction — F_max = μ_s·N

  4. Substituting

  5. Driving component — W·sin θ = 834·sin 28° = 391.5 lb

  6. Compare — 391.5 > 184.1 → slips without restraint

  7. Push to move up — P = W·sin θ + μN = 575.6 lb

Answer: Slips; P ≈ 575.6 lb to move it up

Why the other options are there

  • 208.5 lb (weight used as the normal force)
  • 207.4 lb (friction sign reversed)

Reference: FE Reference Handbook — Statics → Belt Friction

Example 7
Torque to raise a load on a square screw thread — Belt Friction (3)

A screw jack with a mean thread diameter of 2.50 in and a lead of 0.30 in per turn raises a 20,000 lb load. The coefficient of friction on the screw thread is 0.12. Find the required torque.

Given

  • W = 20,000 lb
  • d_m = 2.50 in
  • L = 0.30 in
  • μ = 0.12

Find

Torque required to raise the load

Start with the thinking

  • The screw thread is an inclined plane wrapped around a cylinder — the lead angle comes from the lead over the mean circumference.
  • Raising adds the friction angle to the lead angle; lowering subtracts it.

Step-by-step solution

  1. Formula

  2. Substituting

  3. Friction angle

  4. Formula

  5. Substituting

  6. Evaluate — T = 3,973 in·lb = 331.1 ft·lb

Answer: T ≈ 3,973 in·lb (331.1 ft·lb)

Why the other options are there

  • 954.9 in·lb (friction ignored)
  • 2,036 in·lb (lowering torque)

Reference: FE Reference Handbook — Statics → Belt Friction

Example 8
Impending slip on an inclined plane — Belt Friction (4)

A 371 lb crate rests on a 25° incline with μ_s = 0.35. Does it slip, and what force parallel to the incline is required to start it moving up?

Given

  • W = 371 lb
  • θ = 25°
  • μ_s = 0.35

Find

Slip check and required push

Start with the thinking

  • Compare the driving component to the maximum available friction.
  • Normal force uses the cosine, driving force the sine.
WWNP

Figure for Impending slip on an inclined plane — Belt Friction (4)

Step-by-step solution

  1. Normal force — N = W·cos θ

  2. Substituting — N = 371·cos 25° = 336.2 lb

  3. Maximum friction — F_max = μ_s·N

  4. Substituting

  5. Driving component — W·sin θ = 371·sin 25° = 156.8 lb

  6. Compare — 156.8 > 117.7 → slips without restraint

  7. Push to move up — P = W·sin θ + μN = 274.5 lb

Answer: Slips; P ≈ 274.5 lb to move it up

Why the other options are there

  • 129.9 lb (weight used as the normal force)
  • 39 lb (friction sign reversed)

Reference: FE Reference Handbook — Statics → Belt Friction

Example 9
Torque to raise a load on a square screw thread — Belt Friction (4)

A screw jack with a mean thread diameter of 1.75 in and a lead of 0.40 in per turn raises a 6,000 lb load. The coefficient of friction on the screw thread is 0.24. Find the required torque.

Given

  • W = 6,000 lb
  • d_m = 1.75 in
  • L = 0.40 in
  • μ = 0.24

Find

Torque required to raise the load

Start with the thinking

  • The screw thread is an inclined plane wrapped around a cylinder — the lead angle comes from the lead over the mean circumference.
  • Raising adds the friction angle to the lead angle; lowering subtracts it.

Step-by-step solution

  1. Formula

  2. Substituting

  3. Friction angle

  4. Formula

  5. Substituting

  6. Evaluate — T = 1,671 in·lb = 139.3 ft·lb

Answer: T ≈ 1,671 in·lb (139.3 ft·lb)

Why the other options are there

  • 382.0 in·lb (friction ignored)
  • 863.0 in·lb (lowering torque)

Reference: FE Reference Handbook — Statics → Belt Friction

Example 10
Impending slip on an inclined plane — Belt Friction (5)

A 339 lb crate rests on a 10° incline with μ_s = 0.35. Does it slip, and what force parallel to the incline is required to start it moving up?

Given

  • W = 339 lb
  • θ = 10°
  • μ_s = 0.35

Find

Slip check and required push

Start with the thinking

  • Compare the driving component to the maximum available friction.
  • Normal force uses the cosine, driving force the sine.
WWNP

Figure for Impending slip on an inclined plane — Belt Friction (5)

Step-by-step solution

  1. Normal force — N = W·cos θ

  2. Substituting — N = 339·cos 10° = 333.8 lb

  3. Maximum friction — F_max = μ_s·N

  4. Substituting

  5. Driving component — W·sin θ = 339·sin 10° = 58.9 lb

  6. Compare — 58.9 < 116.8 → stays in place

  7. Push to move up — P = W·sin θ + μN = 175.7 lb

Answer: Stable; P ≈ 175.7 lb to move it up

Why the other options are there

  • 118.6 lb (weight used as the normal force)
  • -58 lb (friction sign reversed)

Reference: FE Reference Handbook — Statics → Belt Friction

Self-check

Answer these without notes before moving on.

  1. Without looking, state the relation on this page whose left-hand side is the quantity most often requested, and name every symbol in it.
  2. Which assumption, if violated, makes the main relation of this section invalid?
  3. Given a determinate frame, truss or beam in equilibrium, what is the first quantity you would compute, and why that one first?
  4. Which unit conversion in this subject most often produces a wrong answer choice, and what is its numerical factor?
  5. Rework Example 1 above from the givens alone, without reading the solution lines.

Chapter summary

  • Belt Friction contains 5 relations; you must be able to find this page in under 15 seconds.
  • Exam style: one free body, three equilibrium equations, one unknown reported.
  • Unit rule: keep force in lbf or kN and distance in ft or m consistently.
  • Work the 10 examples until the solution path, not the answer, is automatic.

Common traps in this section

  • keep force in lbf or kN and distance in ft or m consistently
  • Answering the intermediate quantity instead of the quantity requested.
  • Rounding intermediate values before the final step.
  • Using a relation from an adjacent handbook section that shares a symbol.
  • Skipping the sketch — most lost points on this page start with a misread geometry.
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