Flywheel Energy Storage and Crankshaft Torque Curves in Mechanical Presses
Why the Electric Motor Doesn't Punch the Metal
A common operational myth is that the electric drive motor supplies punching power during impact. In truth, the motor's sole job is to accelerate and replenish kinetic energy in the rotating flywheel during the idle portion of the stroke. The flywheel acts as a mechanical capacitor.
Kinetic Energy Equation for Press Flywheels
Kinetic Energy (E) = 0.5 × I × ω²
Where I is the moment of inertia ($kg cdot m^2$) and $omega$ is rotational velocity ($rad/sec$). During penetration, the flywheel slows down (typically by $10\% ext{ to }15\%$), giving up its stored momentum to push the ram through the work hardening point.
Flywheel Recovery vs Motor Slip
| Operational Metric | Correctly Sized Heavy Flywheel | Undersized / Inefficient Flywheel |
|---|---|---|
| Speed Drop during Piercing | 8% - 13% Nominal | Exceeds 25% (Motor Stalling) |
| Motor Current Spikes | Smooth, regulated load current | Overheating, tripped thermal overloads |
| Cycle Speed Consistency | Constant SPM across batch runs | Sluggish return, uneven part draw |
Rated Tonnage Distance Above Bottom Dead Center (BDC)
Mechanical presses deliver their full rated tonnage only within a narrow window—typically $3.2 ext{ mm to }6.3 ext{ mm}$ above BDC. Initiating high-load forming higher up the stroke drastically lowers available torque and risks fracturing connecting rod bolts.
Engineered Torque Dynamics
Milap Industrial Corporation balances all flywheels dynamically on digital CNC balancers to guarantee zero radial whip at continuous top speeds.
Technical Inquiries: info@milap.net