planetary reducer gearbox

Key feature:
Planetary gearbox is made by modular design, and may be mixed according to client’s request
Involuted planetary gear design
Nodular cast iron Housing to improve rigidity and antiknock
Durable bearing on low‐quickness shaft, and can bear big radial load because of proportionate distribution of torque
All gears are case hardened to get high surface hardness, which guarantee transmission efficiency and whole gearbox’s life
Planetary gearbox has 16 models for different torque range, and each model have 1‐5 reduction stages to accomplish different ratios
Ratio range: 3.15‐9000
Input power: 0.25‐55KW
Permit torque rang: ≤ 800000N. M
Output speed: 0.425‐445 r/min
Structure mode: Chance for flange, foot, or shaft mounting solutions
Wide and comprehensive range of N series for industrial applications
Low speed shaft design: Cylindrical with important, splined, hollow with shrink disc or splined hollow shaft
Rigid and specific nodular cast iron casing
Low noise working, high manufacturing quality standard
High and reliable performance, load capacity and low speed shaft bearing

Ideal for servo applications, the P Series Inline EP Precision Gearhead feature planetary gearing and bearing options to create them the most accurate and efficient planetary gearheads available. Our gear technology provides minimum put on, low noise, and backlash of ≤3 arcmin. The P Series swiftness reducer can be mounted on nearly every servo motor.

For application & selection assistance, please call, fax or email us. Your application info will be examined by our engineers, who’ll recommend the very best solution for the application.
EP precision planetary gearboxes work very well for increasing torque output of servo systems, whilst reducing the reflected load inertia for higher response. Offered in inline, right-angle and hub designs, these best-in-class gearboxes provide high stiffness, high efficiency, and incredibly quiet operation. Mounting equipment is included for mating to EP motors.

These reducers are typically selected predicated on the peak cycle forces, which usually happen during accelerations and decelerations. These cycle forces rely on the driven load, the acceleration vs. time profile for the cycle, and any other exterior forces functioning on the axis.

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