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This expression implies that the load inertia should be made equivalent to the motor inertia by appropriate gearing, in order to obtain the best acceleration Substituting equation 1821 in 1820, we can show that the maximum acceleration is given by max = 1 Tm peak L 2 Jm r (1822)

Equations 1816 through 1822 are very useful in sizing a motor and in determining whether any gearing will be necessary to achieve the desired performance

Dwarf Plants 277 1/4 266 11 121 0.45

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Although the de nition of various torques was introduced in 17, it will be useful to brie y review these de nitions in light of the preceding subsection In sizing a motor, it is important to ensure that the motor is capable of overcoming the static friction at start-up, to accelerate to the desired speed in an acceptable fashion, and to handle any overloads that may occur The following de nitions will help in the analysis: 1 Locked-rotor, or static, torque: The minimum torque the motor will develop at rest for all angular positions under rated conditions 2 Breakdown torque: The maximum torque a motor will develop under rated conditions without an abrupt drop in speed 3 Full-load torque: The torque necessary to produce rated power output at full-load speed 4 Acceleration torque: At any speci ed speed, acceleration torque, ie, the torque available for acceleration, is Tacc = Tm TL TF , where Tm is the motor torque, TL is the load torque, and TF is the frictional load torque Clearly, in order for the motor to accelerate to full-speed operation, the motor torque at standstill must exceed the total static-load torque When the motor torque-speed curve intersects the load torque-speed curve, then a balanced operating condition has been reached

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The equation that de nes the acceleration characteristics of a motor-load pair is Tm T L = J d dt (1823)

Total 1,064 1,064

where TL is the total load torque From this equation we can calculate the time required to accelerate the load from a speed 1 to a speed 2 as follows: t =J

Total 1,064 1,064

2 1

Laramore, R D, 213, 216 Lawn, B R, 121, 123, 139 Lee & Shafer model, 89 Lee, J B, 366, 368, 369, 385, 387, 388, 406 Lee, S C, 403, 407 Lei, G T K, 400 402, 407 Lewis, T G, 169, 170, 173, 185 Li, J, 165, 184 Li, J C M, 165, 184 Li, W, 65, 184 Lim, H S, 164, 185 Limura, Y, 176, 177, 178, 185 Lin, W, 165, 184 Lindberg, R A, 15, 31, 143, 159, 147, 162, 183 185 Linke, T, 305, 362 Logitech, 23 Lowe, I R G, 316, 356, 361 Lubarsky, S V, 170, 185 Lucca, D A, 124, 139, 176, 185

(1824)

787 3/4 798 11 121 0.15

or, in units of rev/min, t= 2 JT (n1 n2 ) (s) 60T (1825)

where T is the net torque (motor torque minus load torque) and JT is the total system inertia (motor inertia plus re ected load inertia)

Probabilities Degrees of Freedom 1 2 3 4 5 6 7 8 9 10 15 20 25 30 0.99 0.000 0.020 0.115 0.297 0.554 0.872 1.239 1.646 2.088 2.558 5.229 8.260 11.524 14.953 0.95 0.004 0.103 0.352 0.711 1.145 1.635 2.167 2.733 3.325 3.940 7.261 10.851 14.611 18.493 0.80 0.064 0.446 1.005 1.649 2.343 3.070 3.822 4.594 5.380 6.179 10.307 14.578 18.940 23.364 0.50 0.455 1.386 2.366 3.357 4.351 5.348 6.346 7.344 8.343 9.342 14.339 19.337 24.337 29.336 0.20 1.642 3.219 4.642 5.989 7.289 8.558 9.803 11.030 12.242 13.442 19.311 25.038 30.675 36.250 0.05 3.841 5.991 7.815 9.488 11.070 12.592 14.067 15.507 16.919 18.307 24.996 31.410 37.652 43.773 0.01 6.635 9.210 11.345 13.277 15.086 16.812 18.475 20.090 21.666 23.209 30.578 37.566 44.314 50.892

The ef ciency of a motor is the ratio of the mechanical power output to the electrical power input, that is, the effectiveness of the electromechanical energy conversion We have already discussed the sources of loss in 17 and classi ed them

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