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s.p.b. Patel engineering college Subject: Dc Machine & Transformer Topic : speed control of dc machine Branch : electrical Prepared by, Shah yash h. (130390109058) guided by, Prof. Malay bhatt prof. manish patel Methods of Speed Control Armature Voltage Control Field Flux Control V Ra m T 2 K e K e Armature Resistance Control Armature Voltage Control 1.Controlled Rectfier V Ra m T K e K e 2 2. Chopper (DC-DC Converter) Field Flux Control Armature Resistance Control Separately or shunt field m V Ra Rext m T K e K e 2 m TR Increasing Re Re Torque Armature Resistance Control V 1 Ra m Series field m Ke K f T Increasing Re Torque Ke K f SPEED CONTROL of SHUNT DC MOTOR • • Two common methods: 1- Adjusting the field resistance RF (and thus the field flux) 2- Adjusting the terminal voltage applied to the armature Less common method: 3- Inserting a resistor in series with the armature circuit SPEED CONTROL of SHUNT DC MOTOR • Changing the Field Resistance • If the field resistance increases, field current decreases (IF↓ = VT/RF↑), and as the field current decreases, flux decreases as well. • A decrease in flux causes an instantaneous decrease in the internal generated voltage EA↓ (=Kφ↓ω), which causes a large increase in the machine’s armature current since VT E A I A RA SPEED CONTROL of SHUNT DC MOTOR • Induced torque in a motor is given by ind =KφIA since flux in machine decreases while current IA increases, which way does the induced torque change? Look at this example: • armature current flow is IA=(250V-245V)/ 0.25Ω= 20A SPEED CONTROL of SHUNT DC MOTOR • What happens in this motor if there is a 1% decrease in flux? • If the flux decrease by 1%, then EA must decrease by 1% too, because EA = Kφω Therefore, EA will drop to: EA2 = 0.99 EA1 = 0.99 (245) = 242.55 V • armature current must then rise to IA = (250-242.55)/0.25 = 29.8 A • Thus, a 1% decrease in flux produced a 49% increase in armature current SPEED CONTROL of SHUNT DC MOTOR • back to original discussion, the increase in current predominates over the decrease in flux so, ind>load , the motor speeds up • However, as the motor speeds up, EA rises, causing IA to fall. Thus, induced torque ind drops too, and finally ind equals load at a higher steady-sate speed than originally • Summarizing behaviour: 1- increasing RF causes IF (=VT/RF) to decrease 2- decreasing IF decrease φ SPEED CONTROL of SHUNT DC MOTOR 3 – Decreasing φ lowers EA(=Kφω) 4 - Decreasing EA increases IA (=VT-EA)/RA 5- increasing IA increases Tind (=KφIA), with change in IA dominant over change in flux 6-increasing Tind makes Tind>Tload & speed ω increases 7-increase in ω, increases EA= Kφω again 8-increasing EA decreases IA 9-Decreasing IA decreases Tind until Tind=Tload at a higher ω • Effect of increasing RF on O/P characteristic of a shunt motor shown in next figure SPEED CONTROL of SHUNT DC MOTOR • Effect of RF speed control on a shunt motor’s torque-speed (over motor’s normal operating range) SPEED CONTROL of SHUNT DC MOTOR • Effect of RF speed control on a shunt motor’s torque-speed (over entire range from no-load to stall conditions) SPEED CONTROL of SHUNT DC MOTOR • According to equation of speed presented before: (a) no-load speed is proportional to reciprocal of flux in motor (b) while slope of the curve is proportional to reciprocal of flux squared • Therefore a decrease in flux causes slope of torquespeed to become steeper • over this range, an increase in field resistance increases motor’s speed • For motors operating between no-load & full-load conditions, an increase in RF may reliably be expected to increase operating speed SPEED CONTROL of SHUNT DC MOTOR • In previous figure (b) terminal characteristic of motor over full range from no-load to stall shown • In figure can see at very slow speeds, an increase in field resistance will actually decrease speed of motor • This effect occurs because at very low speeds, the increase in armature current caused by decrease in EA not enough to compensate for decrease in flux in induced torque field resistance • Some small dc motors used for control purposes operate at speeds close to stall conditions • For these motors, an increase in RF might have no effect or it might even decrease speed of motor • Since the results are not predictable, field resistance speed control should not be used in these types of dc motors. Instead, the armature voltage method should be employed SPEED CONTROL of SHUNT DC MOTOR • CHANGING ARMATURE VOLTAGE • This method involves changing the voltage applied to the armature of the motor without changing the voltage applied to the field • If the voltage VA is increased, then the IA must rise [ IA = (VA ↑ -EA)/RA]. As IA increases, the induced torque ind =KφIA↑ increases, making ind > load , and the speed of the motor increases • But, as the speed increases, the EA (=Kφω↑) increases, causing the armature current to decrease This decrease in IA decreases the induced torque, causing ind = load at a higher rotational speed SPEED CONTROL of SHUNT DC MOTOR • Effect of armature voltage speed control SPEED CONTROL of SHUNT DC MOTOR • Inserting a Resistor in Series with the Armature Circuit • If a resistor is inserted in series with the armature circuit, the effect is to drastically increase the slope of the motor’s torque-speed characteristic, making it operate more slowly if loaded. This fact can be seen from the speed equation: VT RA 2 ind K ( K ) • The insertion of a resistor is a very wasteful method of speed control, since the losses in the inserted resistor are very large. For this reason, it is rarely used