f = n · z / 60
z teeth engage per revolution; the excitation frequency rises proportionally with speed or tooth count.
z teeth engage per revolution; the excitation frequency rises proportionally with speed or tooth count.
Select a target and calculate.
z teeth engage per revolution; the excitation frequency rises proportionally with speed or tooth count.
3,000 rpm and 20 teeth give f = 3,000 · 20 / 60 = 1,000 Hz.
Uniform tooth pitch and speed; actual noise excitation additionally depends on belt tension, tooth profile and structural resonances.
This calculator finds a timing-belt pulley's tooth mesh frequency from rotational speed and tooth count — a figure used to place noise and vibration excitation from timing-belt drives.
Each revolution of a timing-belt pulley, exactly z teeth engage the belt in sequence. At rotational speed n this gives a base mesh frequency f = n·z/60, with n in rpm and f in Hz — the number of tooth engagements per second.
This is similar to a ratchet clicking through a gear: each tooth produces a short impulse, and the click rate rises with speed or tooth count. In timing belts, this impulse train shows up as a tonal excitation that, depending on frequency, can be heard as a hum or whine.
f = n · z / 60
f = n · z / 60n = f · 60/zz = f · 60/n| Symbol / input | Meaning |
|---|---|
| Tooth mesh frequency f | Number of tooth engagements per second at the pulley considered. |
| Rotational speed n | Rotational speed of the timing-belt pulley considered. |
| Tooth count z | Tooth count of the pulley considered. |
Rotational speed n and tooth count z of the pulley considered set the mesh frequency. For a sizing question — at what speed a given excitation frequency should be avoided — n can be chosen as the target.
Enter speed and tooth count of the pulley considered to compute mesh frequency. To avoid a critical frequency such as a housing resonance, choose n as the target and enter the frequency to avoid along with tooth count.
3,000 rpm and 20 teeth give f = 3,000 · 20 / 60 = 1,000 Hz.
A mesh frequency of 1,000 Hz falls in a clearly audible range; if it coincides with a resonance of the housing, mount or an attached component, noise can be markedly amplified.
Rotational speed is given in rpm, tooth count is dimensionless, and mesh frequency is given in Hz.
Because a timing belt runs with constant tooth pitch throughout, the same number of belt teeth engages each pulley in the same time interval, regardless of that pulley's own tooth count. So n1·z1/60 at the driving pulley and n2·z2/60 at the driven pulley give the same numeric value, even though the two pulleys can have different speeds and tooth counts. This shared frequency is the base excitation present throughout the drivetrain.
The calculation is used for the acoustic design of timing-belt drives, for example choosing an operating speed whose mesh frequency avoids a known structural or housing resonance, and for diagnosing noise issues from a measured frequency.
The model gives only the geometrically determined base frequency of tooth engagement. Actual noise generation additionally depends on belt tension, tooth profile geometry, misalignment and the natural frequencies of the surrounding structure, none of which are captured here.
Common mistake: A common mistake is confusing mesh frequency with the plain rotational frequency n/60 — only multiplying by tooth count gives the actual tooth-engagement excitation frequency. It is also easy to overlook that the driving and driven pulleys share the same mesh frequency despite different tooth counts and speeds, since both are driven synchronously by the same belt.
It is the number of tooth engagements between belt and pulley per second, and therefore the geometric base frequency of excitation from a timing-belt drive.
Because the same belt drives both pulleys synchronously, letting the same number of teeth engage each pulley in the same time span, regardless of their individual tooth counts.
If mesh frequency coincides with a natural frequency of the housing or mount, resonance can markedly amplify noise; avoiding such coincidences is a common acoustic design goal.
Belt tension, tooth profile geometry, misalignment and the actual natural frequencies of the surrounding structure, which additionally shape real-world noise generation.
Choose n as the target, enter the frequency to avoid and the tooth count, then pick an operating speed with sufficient margin from that value.