Power Screws and Lead Screws

Thread geometry, torque to raise and lower a load, efficiency, self-locking and ball screws.

What a power screw does

A power screw turns rotation into straight-line motion and a small torque into a large axial force: jacks, presses, vices, valve actuators, machine tool slides and linear stages. The mechanical advantage is large (the force is 2π ÷ lead times the torque, less friction) and the motion slow and smooth. The cost is efficiency: a sliding screw is only 25 to 45 percent efficient, a ball screw 90 percent. The screw’s counterpart in Motion Control and Actuators is the ball screw axis (see the sizing page there); this page gives the machine-element view of the thread, friction and limits.

Thread geometry

The pitch p is the distance between adjacent threads; the lead l is the distance the nut moves in one revolution (l = p for a single-start thread, 2p for a double start). The lead angle is λ = arctan(l ÷ (π dm)), with dm the mean (pitch) diameter. A trapezoidal Tr 30 × 6 screw has a major diameter of 30 mm, a pitch of 6 mm, a mean diameter dm = 30 − 6 ÷ 2 = 27 mm, a lead angle of λ = arctan(6 ÷ (π × 27)) = 4.05° and a root (minor) diameter of 23 to 24 mm.

Torque to raise and lower a load

Traise = (W dm ÷ 2) × (l + π μ dm) ÷ (π dm − μ l)    Tlower = (W dm ÷ 2) × (π μ dm − l) ÷ (π dm + μ l)

Worked example: the press stop screw

Worked example: a Tr 30 × 6 screw raising 10 kN against the press stop

  • Mean diameter 27 mm, lead 6 mm: λ = 4.05° (tan λ = 0.0707).
  • With μ = 0.15 (steel on bronze, lubricated): Traise = 10 kN × 13.5 mm × (6 + π × 0.15 × 27) ÷ (π × 27 − 0.15 × 6) = 30.1 N·m at the thread.
  • Efficiency of the thread e = W l ÷ (2π T) = 10 000 × 6 ÷ (2π × 30 119) = 32 percent; the other 68 percent is friction heat.
  • Collar friction (a thrust washer with μc = 0.10 at a mean radius of 20 mm): Tc = 0.10 × 10 000 × 20 = 20.0 N·m. Total torque 50.1 N·m, overall efficiency 19 percent. A ball thrust bearing would cut the collar term to under 1 N·m.
  • Speed and power: at 300 rpm the nut moves 30 mm/s; the input power is T ω = 50.1 × 31.4 = 1 575 W, while the useful power is W v = 300 W: the difference is heat in the nut (check the nut’s pressure-velocity limit with the maker).
  • Lowering: Tlower = 10.6 N·m is positive, so the load does not drive the screw back down: the screw is self-locking.

Efficiency and self-locking

The screw self-locks (holds the load with no brake) when the friction angle exceeds the lead angle, i.e. μ > tan λ. Here μ = 0.15 > 0.071: it locks. The consequence is a trade-off: a screw that holds its load has an efficiency below 50 percent. An efficient screw (ball screw, or a steep lead) will back-drive: the load turns it, so the drive needs a brake or a worm stage. Vibration can unlock a marginally self-locking screw; for hoisting use a brake or a second locking element.

Power screw efficiency against lead angle051015202530020406080100lead angle (degrees)efficiency (%)ball screw μ = 0.01lubricated acme μ = 0.08dry or poor μ = 0.15Tr 30 × 6: 4.0°, 32 %e = tan λ (1 − μ tan λ) ÷ (tan λ + μ), ignoring the collar. A screw self-locks (cannot be back-driven) whenμ > tan λ, which is why the efficient designs are not self-locking.
Screw efficiency against lead angle for three friction coefficients.

Ball screws

A ball screw replaces sliding with rolling: recirculating steel balls between the nut and screw. Friction coefficient falls to 0.005 to 0.02, efficiency to about 90 percent, and wear and backlash are low (preloaded nuts remove the backlash). The torque for the same load: T = W l ÷ (2π e).

Worked example: a ball screw in place of the Acme screw

  • The 6 mm lead ball screw at e = 0.90 needs T = 10 000 × 6 ÷ (2π × 0.90) = 10.6 N·m, 0.2 times less than the 50.1 N·m of the Acme screw with its collar (4.7× the torque), so a much smaller motor and no heating problem.
  • A 10 mm lead ball screw needs 17.7 N·m for the same load but moves 10 mm per turn: 1.7 times the speed per rpm.
  • Back-driving: the load drives the 10 mm lead screw back with a torque of W l e ÷ (2π) = 14.3 N·m: a vertical axis needs a brake (a spring-applied holding brake on the motor) or it falls when the power fails.

Buckling, critical speed and thread stress

  • Column buckling: a long screw in compression buckles like a column: Pcr = π² E I ÷ L² for pinned ends, with I from the root diameter. For dr = 24 mm and L = 500 mm: I = 16 286 mm⁴, Pcr = 135 kN (540 kN with fixed ends): against 10 kN a factor of 13.5 for the pinned case; use a safety factor of at least 3 to 5 (see Columns and Buckling).
  • Critical speed: a long, rotating screw whips at its natural frequency. For a 26 mm root diameter screw 1 m between pinned supports, ω = (π ÷ L)² × (dr ÷ 4) √(E ÷ ρ) = 332 rad/s = 3 169 rpm; run below 80 percent of that: 2 535 rpm, i.e. 25.3 m/min with a 10 mm lead. Fixed ends raise the limit by 1.5 to 2.2 times (see Vibration, Isolation and Noise).
  • Thread stress: axial stress in the root area 661 mm² is 15 MPa (plus torsion); the bearing pressure on the nut thread: W ÷ (π dm × thread depth × number of threads) ≈ 6.5 MPa for a 36 mm nut, below the 5 to 10 MPa limit for bronze (3 to 5 for a polymer nut).
  • Wear and lubrication: use a lubricant film and a nut of bronze or filled plastic that wears before the screw; backlash grows with wear (a split nut or a spring-loaded one takes it up).

Choosing a screw

TypeFriction μEfficiencyNotes
Square0.10 to 0.2035 to 50 %rarely made now; high strength; difficult to adjust for wear
Acme / trapezoidal (Tr)0.10 to 0.2025 to 45 %the common lead screw; split nuts take up wear; self-locking at low leads
Buttress0.10 to 0.2030 to 50 %one-way heavy thrust (presses, vices)
Ball screw0.005 to 0.0285 to 95 %recirculating balls; precise; not self-locking; needs a brake
Roller screw0.003 to 0.0185 to 95 %highest load, speed and life; expensive

Related

FAQ

What is the difference between pitch and lead?

Pitch is the spacing of the thread; lead is the travel per revolution. They are equal for a single-start thread; a two-start thread has a lead of twice the pitch.

Can I back-drive a lead screw?

Not if it self-locks (μ > tan λ): that is why jacks hold. A ball screw or a steep-lead screw will back-drive and needs a brake.

Why does my screw get hot?

Friction: a sliding screw dissipates 55 to 75 percent of the input power. Reduce the speed, lubricate, use a better nut material or a ball screw.

Why does the axis wobble at speed?

You are near the critical speed of the screw. Shorten the span, increase the diameter, support the far end or reduce the speed.

References

  • Shigley, J. E., Mischke, C. R., Budynas, R. G., Mechanical Engineering Design, McGraw-Hill (power screws); Norton, R. L., Machine Design, Pearson.
  • ISO 2904 (trapezoidal thread profile), ISO 3408 (ball screws), DIN 103 (Tr threads); THK, NSK, Hiwin and Bosch Rexroth ball screw catalogs.
  • Machinery’s Handbook, Industrial Press (screw threads, Acme and trapezoidal).

Last reviewed: October 2026. Friction coefficients and efficiencies are typical for lubricated screws.