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ET 332a Dc Motors, Generators and Energy Conversion Devices 1.

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Presentation on theme: "ET 332a Dc Motors, Generators and Energy Conversion Devices 1."— Presentation transcript:

1 ET 332a Dc Motors, Generators and Energy Conversion Devices 1

2 Learning Objectives After this presentation you will be able to:  Compute the average output voltage of a dc generator given machine physical construction parameters.  Draw the schematic circuit model of a dc machine  Find generator output voltage using a magnetization curve and defining formulas.  Compute generator voltage regulation. 2

3 Average Induced Voltage in a Generator 3 Where v = velocity of conductor For rotating system v = angular velocity d  /dt =  rad/s Start with fundamental equation Frequency of e related to number of field poles and rotational speed by: Angular velocity relates to frequency f (cycles/s or Hertz) by:  = 2  f Where: P = number of field poles n = rotational speed (rpm)

4 4 Average Induced Voltage in a Generator Substituting into fundamental equation and simplifying gives: Where: P = number of poles n = rotational speed N a = # of turns in coil  p = field flux E a = average induced voltage Consider machine construction details and define another voltage formula

5 5 Average Induced Voltage in a Generator Define the number of conductors in field in terms of windings z a = Total number of armature conductors in the field. Substitute into previous equation to get: Where: a = number of parallel paths

6 6 Average Induced Voltage in a Generator The number of poles, parallel paths, and conductors are constant once the machine is constructed so define: The constant k G also known as k e in some texts. Relates motor voltage to speed and field flux. Where k G = emf constant Note : E a is proportional to the flux and to the rotational speed. If conditions of machine are know at one n and  p, another operating point can be found by equating ratios.

7 Induced Voltage Examples 7 Example 1: A 2 pole dc motor armature rotates at 1800 rpm. It has 400 turns in the armature winding. The magnetic field flux is 0.0025 Wb. Compute the average induced voltage. Example 2: A 4 pole dc machine rotates at 200 rad/s in a magnetic field of 0.0048 Wb. There are 4 parallel current paths that have 200 conductors. Find the induced voltage in the armature and the emf constant for the machine. Convert  o n for formula

8 8 Induced Voltage Examples Example 2 Continued: Find the emf constant Lump the constants and compute Example 3: A 4 pole 50 kW dc machine has a value of E a = 110 V at 1100 rpm. What is the induced voltage if the speed is increased 20%? No change in flux Find E a2 Ans

9 9 Induced Voltage Examples Example 4: A 4 pole dc machine has a value of E a = 50 V at 400 rpm. What is the value of E a if the pole flux is doubled while the speed remains constant? Assumes no saturation Ans

10 10 Circuit Model of Dc Machines R acir = dc resistance of the armature windings, interpoles, etc L a = inductance of armature circuit R f = dc resistance of the field windings L f = inductance of the field windings E a = internally induced voltage V t = terminal voltage of machine V f = field electromagnetic source voltage VfVf + EaEa + VtVt + LfLf LaLa RfRf R acir Inductances have no effect when the values of dc current are not changing. Shown to indicate coils.

11 Generator Circuit Model 11 EaEa + LfLf LaLa RfRf R acir VfVf IaIa VtVt + Generator model - mechanical power converted to electric power. I a leaves the + terminal of armature IfIf Field current produces field flux From KVL around armature circuit Total resistance of armature circuit R acir Where: R a = armature resistance R IP = interpole winding resistance R cw = compensation winding resistance Brush losses P=2 ∙I a 1 volt drop for each brush Brush drop

12 12 Motor Circuit Model EaEa + LfLf LaLa RfRf R acir VfVf IaIa IfIf Brush drop VtVt + Motor model - electric power converted to mechanical power. I a enters the + terminal of armature Analyze the field circuit Control I f with field rheostat IfIf R c = field coil resistance R f = field rheostat resistance

13 Separately Excited Dc Generator 13 R acir LaLa EaEa LfLf RcRc RfRf VfVf VtVt N n Separate source of supply develops field flux. Source called the exciter RLRL Model Equations: Field circuit current Magnetic coupling to induced average voltage E a in terms of flux for constant I f pp E a proportional to n for constant I f IfIf

14 14 Separately Excited Dc Generator Generally flux,  is non-linear with respect to the field current I f. Magnetizing curve for generator gives relationship for E a as a function of field current. If I f is in linear part of curve E a is proportional to n and I f. Field Current, I f (A) Induced EMF, E a (V) k e valid here Generator Magnetizing Curve

15 Terminal Voltage Regulation 15 Voltage regulation finds the percent change in terminal voltage from no- load to full load VtVt KVL around armature circuit with switch closed IaIa n With switch closed and n constant V t < E a and decreases as I a increases I a = 0 with switch open so:No-load voltage = E a

16 16 Terminal Voltage Regulation For rated terminal voltage Where:%VR = percent voltage regulation V nl = no-load terminal voltage V rated = name plate rating of the terminal voltage when generator delivers rated power. How does terminal voltage change with delivered power?

17 17 Terminal Voltage Regulation IaIa EaEa I a, rated V rated V nl R acir Generator Terminal Voltage Vs Load Current Equation above plots as downward sloping line for changes in armature current I a = 0 As armature current decreases (load decreases)Terminal voltage increases (V t increases) %VR related to the armature circuit voltage drop. Smaller %VR is better.

18 Voltage Regulation Example 18 Example 1 A separately excited 50 kW, 3500 rpm, 2-pole dc generator has a rated terminal voltage of 120 Vdc. Its exciter is supplied from a 120 Vdc supply. The field coil resistance is 10.4  and the field rheostat is set at 20.5 . The total armature resistance is 0.014 . The generator is supplying 420 A to a load. The magnetizing curve is given on a previous slide. Determine: a.) the induced armature voltage at this level of excitation b.) the terminal voltage at 100%, 75% and 50% load current

19 Voltage Regulation Solution 19 Draw schematic model for generator Use I f and magnetization curve to find E a E a =162 V I f =3.88 A

20 20 Voltage Regulation Solution Solution continued: Compute regulation at different load levels

21 21 Voltage Regulation Solution Solution continued: Compute regulation at different load levels Summary of calculations % LoadIaIa VtVt 100420 A156.12 75315 A157.59 V 50210 A 159.86 V Terminal voltage increases on generator as the load current decreases

22 22 Example 2: For the machine in Example 1,,determine the field rheostat setting for the machine to deliver rated output current at rated voltage. Also determine the %VR at rated load. Separately Excited Generator Example Solution Calculate the current at rated load for the generator power rating Find Rated I from power and voltage Now find value of E a with V t = 120 V using

23 23 Separately Excited Generator Example Example 2 Continued Use magnetization curve to find I f E a =162 V I f =3.88 A E a =125.8 V I f =2.8 A I f = 2.8 A from graph. Now find R f Solve for R f

24 24 Separately Excited Generator Example Example 2 Continued From Previous example Find the % VR Percent Voltage Regulation V nl = V t with I a =0 V nl =125.833

25 ET 332a Dc Motors, Generators and Energy Conversion Devices 25


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