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Pulley shaft load from belt span tensions

Shaft load is the vector resultant of both span tensions, not their effective-force difference.

MINTSI
01

Inputs

Force resultant acting on pulley hub, shaft and bearings.

Force in the more highly loaded belt span.

Force in the less highly loaded belt span.

Angle between the two span-force vectors directed away from the pulley center; for an open two-pulley drive it equals wrap angle at the pulley considered.

02

Result

Select a target and calculate.

Calculation

FW = √(F₁² + F₂² − 2F₁F₂ cos β)

Shaft load is the vector resultant of both span tensions, not their effective-force difference.

Understand the inputs
  • Resultant shaft load FWForce resultant acting on pulley hub, shaft and bearings.
  • Tight-side tension F₁Force in the more highly loaded belt span.
  • Slack-side tension F₂Force in the less highly loaded belt span.
  • Included span angle βAngle between the two span-force vectors directed away from the pulley center; for an open two-pulley drive it equals wrap angle at the pulley considered.
Example

F₁ = 1,000 N, F₂ = 400 N and β = 165° give FW ≈ 1,390.2 N.

Assumptions and limits

Planar static force resultant at the pulley center; belt weight, axial forces, shock factors and pulley overhang to the bearing are excluded.

Technical article

Understand Pulley shaft load from belt span tensions

This calculator combines tight-side tension, slack-side tension and span angle into the resultant force on a pulley. That shaft load governs bearing and shaft bending and is fundamentally different from the effective tension difference that transmits torque.

What does this quantity describe?

Both belt spans pull along their own directions. The law of cosines gives FW = √(F₁²+F₂²−2F₁F₂ cos β), where β is the angle between span-force vectors directed away from the pulley center.

Two ropes leaving the same ring in nearly opposite directions load the ring by almost the sum of their magnitudes. If they point nearly the same way, the resultant approaches their difference. β captures this directional effect.

Formula and variables

FW = √(F₁² + F₂² − 2F₁F₂ cos β)

  • FW = √(F₁²+F₂²−2F₁F₂ cos β)
  • β = arccos[(F₁²+F₂²−FW²)/(2F₁F₂)]
  • at β = 180°: FW = F₁+F₂
  • at β = 0°: FW = |F₁−F₂|
Symbol / inputMeaning
Resultant shaft load FWForce resultant acting on pulley hub, shaft and bearings.
Tight-side tension F₁Force in the more highly loaded belt span.
Slack-side tension F₂Force in the less highly loaded belt span.
Included span angle βAngle between the two span-force vectors directed away from the pulley center; for an open two-pulley drive it equals wrap angle at the pulley considered.

Choose the inputs correctly

F₁ and F₂ are operating span tensions. β is the included angle of outward force vectors; for a simple open two-pulley drive it equals the wrap angle at the pulley. Confirm the convention with a free-body diagram.

How to use the calculator

Select FW and enter both tensions and β. Use the result as an external radial load in subsequent shaft and bearing analysis, adding actual pulley overhang, load direction, other pulleys and service factors.

Worked example

For F₁ = 1,000 N, F₂ = 400 N and β = 165°, FW = 1,390.2 N. At β = 180° it would be exactly 1,400 N; at β = 0°, 600 N.

Understand the result and units

A 1.39 kN resultant acts at the pulley center. An overhung pulley also creates a bending moment at the bearing. The load direction follows from vector geometry and is not supplied by this magnitude-only result.

Forces use newtons and angles are evaluated in radians internally; degrees can be selected. For a later bending moment, multiply FW by pulley-to-bearing offset in metres.

From pulley force to bearing force

FW is an external force at the pulley center. With a pulley between two bearings, reactions split according to distances. With an overhung pulley outside the bearings, reactions and shaft bending rise. Bearing-life input therefore comes only after resolving all external loads into each bearing reaction.

Typical applications

Shaft load supports bearing-life, shaft-deflection and gearbox overhung-load checks, and shows the effect of changed pretension. Gates explicitly recommends comparing calculated overhung load with the gearbox manufacturer's limit.

Assumptions, limits and common mistakes

This is a planar static resultant. It excludes misalignment axial force, weight, shock/service factors and spatial superposition of other elements. Actual bearing reactions also require bearing locations and static equilibrium.

Common mistake: Do not use F₁−F₂ as bearing load. Do not assume 180° without checking geometry, and do not confuse wrap angle with the smaller angle between tangent lines. Treat forces for multiple belts consistently.

Frequently asked questions

Does shaft load equal F₁ + F₂?

Only at β = 180°. In general, calculate the vector resultant with the law of cosines.

Which angle should I enter?

The angle between both span-force vectors directed away from the pulley center. In a simple open drive it equals pulley wrap angle.

Why can shaft load exceed Fᵤ?

Fᵤ is the torque-producing difference, while both pretensioned spans pull on the shaft and largely add geometrically.

Can FW go straight into a bearing-life calculator?

Only if one bearing truly carries the complete resultant. Usually the force must be combined with other loads and split into two bearing reactions.

How can shaft load be reduced?

Depending on the drive, larger sheaves, appropriate rather than excessive tension, suitable wrap and reduced overhang can help; changes must follow the manufacturer selection.