Speed Regulation Control of DC universal motor for Electric Forklift

1. Voltage regulation and speed regulation of DC universal motor of electric forklift. By changing the voltage Um at the motor end, for example, by swapping batteries in series or parallel; Alternatively, a resistor can be connected in series in the armature circuit, or two motors can be connected in series or parallel to change the speed n. The specific method is shown in the table below.

1. Figure 1 shows the schematic circuit diagram.

Figure 1

When the thyristor V of the DC universal motor of the electric forklift is turned on, its terminal voltage Um is equal to the power supply voltage U; When the thyristor V is turned off, the motor is disconnected from the power supply, and its terminal voltage Um is equal to zero. If the thyristor is periodically turned on and off at a certain speed, the terminal voltage Um of the motor will have a waveform as shown in Figure 2 (b). Assuming that the conduction time t of the thyristor is the width of the conduction time and the turning off time is the width of the turning off time, the average value Um of the motor terminal voltage is:Ump=Ut/ (t+t)=Ut;/ In the formula T=rU, T=ti+t2 is called the working cycle
R=ti/T, which is called the conduction ratio.
Therefore, by changing the conduction ratio of the thyristor, the average terminal voltage of the motor can be changed, thereby achieving the goal of speed regulation. There are three methods to change the conduction ratio:
(1) Fixed frequency and width modulation: the period T is fixed, and the conduction time width t1 is changed
Fixed width frequency modulation: t fixed, changing the cycle T, i.e. changing the operating frequency (2)
(3) Frequency modulation and width modulation: t both change.
The speed regulation methods of fixed frequency width modulation and frequency modulation width modulation mentioned above have been applied in future battery forklift circuits. In practical application circuits, a diode VD is also connected in parallel at both ends of the motor, called a freewheeling diode, as shown in Figure 2.

Figure 2

In this way, when the thyristor V is turned on, the current G supplied by the power supply GB to the motor will increase exponentially, and its waveform is shown in Figure 2-12 (b). When the thyristor V is turned off, the power supply does not supply current, i.e. iGB-0. However, due to the energy stored in the inductance of the motor winding, the motor current continues to flow through the diode VD, meaning that the waveform of the current i flowing through the motor M decreases exponentially. Therefore, the current Im flowing through motor M should be the sum of the power supply current ie and the continuous current i, i.e. Imi+iv, and its waveform is shown in Figure 2. It can be seen that after the DC universal motor of electric forklift is connected in parallel with the freewheeling diode, the conduction of the thyristor can be relatively small。