Edited by John R. Gyorki
|ED NOVAK Aerotech Inc. Pittsburgh, Pa.|
Linear motors are rapidly becoming the technology of choice for motion control in numerous machines, especially for increasing throughput. The speed, acceleration, and positioning accuracy of linear-motor systems are unsurpassed by any other linear-motion technology.
The fundamental equations for calculating the required forces during a trapezoidal move are:
Fa = ma + F
Ft = Ff
Fd = ma + F and
Fw = 0.
where m = mass, kg; a = acceleration, mm/sec/sec; Fa = force required to accelerate the load, lb; Ft = force required during traverse motion of the load, lb; Fd = force required to decelerate the load, lb; Ff = frictional force, lb; and Fw = force at dwell, lb.
The load cannot accelerate instantaneously from 0 to 2m/sec, so apply the equation for the most efficient move — a trapezoidal move with constant acceleration. Divide 250 msec into three equal parts: one-third acceleration, one-third traverse, and onethird deceleration, or 250 msec/3 = 83.3 msec.
This is the peak rating needed from the prospective motor, derived only from acceleration force. It does not account for friction or other opposing forces. For example, a quality cross-roller bearing used to carry the load has a coefficient of friction of about 0.0005 to 0.003. When the 50 kg rides on these bearings, the frictional force is
The frictional force is low because the linear bearings are highly efficient. And because friction always opposes motion, it adds to the driving force required; 405 lb + 0.33 lb = 405.33 lb. Next, with a known total acceleration force, determine the rms or continuous- force requirement. The rms force is the major contributor to the temperature rise of the linear motor’s forcer coil, which ultimately limits the power output. This is where the duty cycle enters the equation. For the example, the duty cycle:
Use the rms force, 227.7 lb, to choose a specific model from a linear motor catalog that can apply this force continuously. Adding air cooling can significantly increase the rms output force of a particular motor which allows a smaller forcer coil to maximize stroke length.