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L6238S Datasheet(PDF) 24 Page - STMicroelectronics |
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L6238S Datasheet(HTML) 24 Page - STMicroelectronics |
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24 / 31 page ![]() The relation between these variables is given by: V = Lmtr dimtr dt Rmtr imtr + Eg (5.1.2) where: V = Applied Voltage imtr = Motor Current Lmtr = Total inductance of the motor windings Rmtr = Resistance in series with the motor Eg = The internally generated voltage of the motor, proportional to the motor velocity Since: Eg =KE ω (5.1.3) The above equations can be combined to form the basic electrical equation for a motor: V = Lmtr dimtr dt Rmtr imtr + KEω (5.1.4) Figure 5.5 is a simplified electrical equivalent of the output stage of the L6238S along with the model of the motor during the time that the Out- put Drives are conducting. The additional resistance associated with the out- put stage and sensing resistor are also in series with the motor. If we let Rs equal the total series resistence: Rs = 2*RdsON +Rmtr +Rsense (5.1.5) then (5.1.4) becomes: V = Lmtr dimtr dt Rs imtr + Eg (5.1.6) Figure 5-6 is an equivalent circuit of the output stage during the Constant-OFF period. During the OFF time the lower driver for the particular phase beign driven remains ON. The internally generated voltage forces the path of current though the motor, its series resistance, the RdsON of the Lower Driver and finally through the opposite lower driver. PWM Example (Refer to Figure 5-7) The following is an example on how to select the timing parameters. Given: DCStart Current = 1.25A Ripple Current = 100mA Duty Cycle = 50% Motor Interface (L) = 880 µH Total Series Resistance (Rs) = 4.8 Ω If the worst case start current is 1.25A and the duty cycle is 50%, then the Peak Current, It will be: it = 1.25+ 0.1 2 it = 1.30A Eg + - Rmtr Lmtr D95IN321 Figure 5-4 + - Rmtr Lmtr D95IN322 UPPER Rdson KEW LOWER Rdson Rsense Figure 5-5 + - Rmtr Lmtr D95IN323 KEW LOWER Rdson LOWER Rdson Figure 5-6 L6238S 24/31 |
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