Some practice problems At end of the module G1 student text are some problems. I suggest that you work on problems 1, 4, 6, and 7. This will provide you.

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Presentation transcript:

Some practice problems At end of the module G1 student text are some problems. I suggest that you work on problems 1, 4, 6, and 7. This will provide you with good practice for this module. I will make the solutions available to you later. It is also possible that I may assign one or more of these problems as an in-class group exercise sometime next week.

The power angle Let’s define the angle that Ef makes with Vt as For generator operation (power supplied by machine), this angle is always positive. For motor operation, this angle is negative.

The power angle Vt Ia XsIa jXsIa Ef This is for generator operation. You should see if you can construct the phasor diagram for motor operation, lagging operation (just reverse the arrow on the current) The power angle is the angle between Vt and Ef, and is the angle of Ef if Vt is reference

Example A 10 MVA, 3 phase, Y-connected, two pole, 60 Hz, 13.8 kV (line to line) generator has a synchronous reactance of 20 ohms per phase. Find the excitation voltage if the generator is operating at rated terminal voltage and supplying (a) 300 Amperes at 30 degrees lagging, (b) 300 Amperes at 30 degrees leading

Example (cont’d) Solution (a) (b) Note: 1) 2) lag case referred as overexcited operation 3) lead case referred as underexcited operation

It is usually the case that excitation voltage Ef is lower in magnitude for leading operation as compared to lagging operation. Vt Ia jXsIa Ef jXsIa Implication: If |Ef| is large (small), relative to |Vt|, machine is probably lagging (leading).

It is usually the case that excitation voltage Ef is lower in magnitude for leading operation as compared to lagging operation, but not always. Vt Ia jXsIa Ef Here note that |Ef| for leading case is larger than for lagging case. This is due to much larger Ia in the leading case.

So how can we tell, using Ef and Vt, whether the generator is lagging or leading? We need to look at power relations for the answer. We will derive power relations that do not require knowledge of the current.

Power relationships Recall the power angle,, as the angle at which the excitation voltage,, leads the terminal voltage,. Therefore, from the circuit…. Ef jXs Zload Vt Ia

Power relationships But

Power relationships (cont’d) Equating real and imaginary parts of equ. 1 and 2 and multiplying both sides of the equations by : (3) (4) Note: reactive power is positive when the machine is operated overexcited, i.e., when it is lagging

Example Find Pout and Qout for the conditions (a) and (b) described in the previous example. Solution: (a)

Example (cont’d) (b)

Example (cont’d) Consider: Why is real power the same under the two conditions? When the generator is operating lagging, is it absorbing vars from or supplying vars to the network? What about when the generator is operating leading? For a particular angle, how are the terms “lagging” and “leading” meaningful with respect to real power? With respect to reactive power?

1.0 power factor condition in terms of Ef, Vt, and delta We have seen that gen lagging operation results in +Qout and leading operation results in -Qout. So 1.0 power factor implies Qout=0. Applying this to reactive power equation:

1.0 power factor condition This is the condition for which the generator is operating at 1.0 power factor.

What about leading/lagging operation? In the final equation on the previous page, just replace the equals sign by > (for lagging) or < (for leading).

Let’s look at the phasor diagrams. Vt Ia jXsIa Ef Vt Ia Ef jXsIa Vt Ia

Generation Operation: Generator pull-out power From equ. 3, the plot of the electric power against the power angle

Generation Operation: Generator pull-out power (cont’d) For simplicity neglect all real power losses associated with: –windage and heat loss in turbine –friction in turbine –friction in generator bearings –winding resistances when operating in steady-state if then decreases while remains unchanged which causes machine to accelerate beyond synchronous speed-i.e. the machine has pulled out or lost synchronism

Example Compute the pull-out power for the two conditions described in Example 2 Solution (a) Overexcited case (lagging): (b) Underexcited case (leading): Note: The limit is lower when the generator is underexcited because is lower