PhysSandbox
Classical MechanicsWaves & SoundElectricity & MagnetismOptics & LightGravity & OrbitsLabs
🌙Astronomy & The Sky🌡️Thermodynamics🌍Biophysics, Fluids & Geoscience📐Math Visualization🔧Engineering🧪Chemistry

Related simulators

Continue with similar topics in this category — or all 85 in Classical Mechanics.

View category →
NewSchool

Capstan (Rope on Cylinder)

Launch Simulator

T₂ = T₁ e^{μφ}: μ, wrap angle φ, top view + T₂/T₁ vs φ graph.

School

Atwood Machine

Launch Simulator

Two masses on a pulley. Adjust masses to see acceleration and tension.

NewSchool

Ballistic Pendulum

Launch Simulator

Bullet hits block: embedded vs e; ω₀ = v/L, θ_max, energy graph.

NewSchool

Forearm Lever (class 3)

Launch Simulator

Elbow fulcrum, load at hand, muscle moment arm — torque estimate.

NewSchool

Blocks & Tackle

Launch Simulator

n supporting strands, same rope tension T, ideal MA = n, F = T.

NewSchool

Bridge Resonance (1-D mode)

Launch Simulator

Damped modal oscillator with harmonic drive: sweep ω near √(k/m) — presets for cadence-like and low-ζ peaks.

PhysSandbox

Interactive physics, chemistry, and engineering simulators for students, teachers, and curious minds.

Physics

  • Classical Mechanics
  • Waves & Sound
  • Electricity & Magnetism

Science

  • Optics & Light
  • Gravity & Orbits
  • Astronomy & The Sky

More

  • Thermodynamics
  • Biophysics, Fluids & Geoscience
  • Math Visualization
  • Engineering
  • Chemistry

© 2026 PhysSandbox. Free interactive science simulators.

PrivacyTermsContact
Home/Classical Mechanics/Belt Drive & Slip

Belt Drive & Slip

Two pulleys: tension difference limited by μ and wrap θ (e^{μθ}); load torque vs τ_max and simple slip on ω₂.

Pulleys & drive

12 cm
18 cm
28 rad/s

Belt friction (flat belt caricature)

180 N
0.32
2.75 rad
8.5 N·m

Uses symmetric tensions T₁ = T₀ + ΔT/2, T₂ = T₀ − ΔT/2 with ΔT = min(τ/R₂, ΔT_max). Limit ΔT_max follows from T₁/T₂ ≤ e^(μθ). If τ needs more than ΔT_max, we show slip and scale ω₂ down (linear teaching model).

Shortcuts

  • •Space — zero phase markers

Measured values

ω₂ (ideal, no slip)18.667 rad/s
ω₂ (with slip model)18.667 rad/s
Max torque τ_max26.804 N·m
Slip?no
Slip estimate0.0 %
ΔT required47.22 N
ΔT max (friction)148.91 N

About this model

A flat open-belt drive is modeled with two cylindrical pulleys. Mean belt tension T₀ and a symmetric tight/slack split T₁ = T₀ + ΔT/2, T₂ = T₀ − ΔT/2 are assumed. The friction limit T₁/T₂ ≤ e^{μθ} caps the transferable tension difference and therefore the torque τ ≈ ΔT·R on the driven wheel. When the requested load torque exceeds this limit, the visualization marks slip and scales the driven angular speed with a simple linear teaching rule.

Who it's for: Intro machine elements and friction drives; complements the capstan rope simulator.

Key terms

  • Euler belt formula
  • wrap angle
  • tension ratio
  • torque capacity
  • belt slip

How it works

Open-belt drive caricature: the driver pulls the tight side, the driven resists with torque τ. Friction over wrap angle θ limits how large the tension difference ΔT = T₁ − T₂ can be before the belt slips on the pulley. The steady-state torque on the driven sheave is approximately τ = ΔT · R₂ when there is no slip; beyond the friction limit, real belts slip, heat up, and wear — here we only show a simple scaled ω₂ to signal overload.

Key equations

T₁/T₂ ≤ e^(μθ) ⇒ ΔT_max = 2T₀(e^(μθ) − 1)/(e^(μθ) + 1) for symmetric ±ΔT/2 about T₀

τ = ΔT · R₂, ω₂/ω₁ = R₁/R₂ when no slip

Frequently asked questions

Why is this not a full conveyor-belt FEA?
Real belts have bending stiffness, creep, and different slip physics on the driver vs driven side. This page isolates the textbook capstan inequality and torque limit from mean tension, which is enough to motivate why preload and friction matter.