Title: Advanced Power Systems
1Advanced Power Systems
- ECE 0909.402-02, 0909.504-02
- Lecture 2 Electric Power Fundamentals
- 29 January 2007
- Dr. Peter Mark Jansson PP PE
- Associate Professor Electrical and Computer
Engineering
2Public service announcement
- How many of you are EITs?
- How many are registered to take the EIT?
- Do yourself a favor
- Enroll and take the test, our ECE students at
Rowan thus far have a 100 pass rate and are well
on their way to becoming PEs - http//www.state.nj.us/lps/ca/pels/pelsinfo.htm
3Aims of Todays Lecture
- Course Training Tours (Find Potential Times)
- Part One Overview of Chapter 1 equations
- Discussion of Articles reviewed
- Your Carbon Footprints
- A summary of ch. 2 concepts
- Effective Values of V and I (rms)
- R, L C in ac circuits
- Power Factor
- Power Triangle Power Factor Correction
- Three-Wire Single Phase Residential Wiring
- Three Phase Systems
- Power Supplies and Power Quality
4Aims of Todays Lecture (cont)
- 15 minute stretch break at 6
- Part Two An intro to ch. 3 concepts
- Early developments
- Electric industry today (NUGS, IPPs, QFs)
- Polyphase synchronous generators
- Heat engines, steam cycles and efficiencies
- GTs, CCs, Baseload Plants and LDCs
- TD
- Regulatory impacts (PUHCA, PURPA, FERC)
5Chapter 1 Equations
6Chapter 1 Equations (2)
7Chapter 1 Equations (3)
8Articles Reviewed
- What did you find?
- What did you learn?
- What do you think?
9What is your Carbon Footprint?
- http//www.carbonfootprint.com/
- http//www.safeclimate.net/calculator/
- http//www.climatecrisis.net/takeaction/carboncalc
ulator/ - http//www.carboncalculator.co.uk/
- http//www.bp.com/
- http//www.southampton-sustainability.org/carbonca
lc.htm - http//carbonfund.org/site/pages/calculator/
- http//www.cleanair-coolplanet.org/action/footprin
t.php - http//www.stopglobalwarming.org/carboncalculator.
asp - http//www.cambridgecarbonfootprint.org.uk/footpri
nt_links.htm - http//www.bestfootforward.com/carbonlife.htm
- http//www.mycarbonfootprint.eu/
- http//www.nativeenergy.com/lifestyle_calc.html
10Chapter Two
- Effective Values of V and I (rms)
- R, L C in ac circuits
- Power Factor
- Power Triangle Power Factor Correction
- Three-Wire Single Phase Residential Wiring
- Three Phase Systems
- Power Supplies and Power Quality
11Sinusoidal Sources
- T is period of oscillation
- f 1/T (frequency)
- Units of Hertz
- Cycles per second
- ? 2?f
- Angular frequency
- Radians per second
- ? phase angle
- Offset from zero
- May be degrees or rads
12effective values of periodic waveforms
- what is the effective voltage of a 120VAC/60Hz
outlet in the walls of your home and in this
building? - What is v(t)?
- What is T?
- What is ??
- What is Vm?
T 1/f 1/60Hz 16.667msecs
Vm ?
? 2?f 2?60 377rads/sec
13effective values of periodic waveforms
To understand what Vm might be we need a good
definition of effective value. The effective
value of a current is the steady current (dc)
that transfers the same amount of average (real)
power as the given varying current. The effective
value of a voltage is the steady voltage (dc)
that transfers the same amount of average (real)
power as the given varying voltage.
14effective values of periodic waveforms
effective value is the square root of the mean
of the squared values also known as (a-k-a) the
root-mean-square
15effective values of periodic waveforms
What is the average value of the square of the
cosine of a sinusoid?
By inspection it is ½, going from 0? 1 and back
again
16effective values of periodic waveforms
Since 120 240VAC are effective values this
means they are root-mean-square (rms) values
So What are the amplitudes of these sinusoidal
waveforms if viewed on a scope?
Vm of 120VAC ? LM1 Vm of 240VAC ? LM2
17NOTE
- In practice, electrical engineers must take care
to notice (or determine) whether a sinusoidal
voltage is being expressed in terms of its
effective value (rms) or its maximum (Vm) value - Generally in
- electronics and communications V is Vm
- power applications and this course V is
Vrms -
- Also in practice, we treat incoming voltage
as having a zero phase angle unless otherwise
specified, current angles are then expressed
w.r.t. voltage
18R, L C in ac circuits
- Voltage across resistors is the same as the
voltage supplied by the source - Phase angle of resulting current is the same as
phase angle of the supply voltage - V and I are considered in phase
- And V RI (where V and I are rms values)
- Power VI (and I2R, V2/R)
19Sample problems
- An electric water heater element provides 4500
watts of real power at 240VAC, what is its
resistance (and current)? - How much power will it provide if the voltage
sags to 210VAC?
Write your answers as LM3
Write your answer as LM4
20Capacitors
- V ZI (1/j?C)I (NOTE Z - j/?C)
- In a purely capacitive circuit the current leads
the voltage by exactly 90o (or voltage lags by
90o) - Average power dissipated by a capacitor is zero
(stores and releases) ideal - Sample exercise what is rms current and i(t) in
a 5 ?F capacitor used to balance the power factor
on a motor in the UK (assume 240V/50Hz)
21Capacitor example
- Sample exercise what is current in a 5?F
capacitor used to balance the power factor on a
motor in the UK (assume 240V/50Hz) - V (1/j?C)I so I Vj?C
- (240)j(2?50)(5x10-6) 0.377j A
22You try it capacitor example
- Sample exercise find the rms current and write
an equation for the current as a function of time
when a 500 nF capacitor is used in a 120VAC/60Hz
system - Remember V (1/j?C)I so I Vj?C
Write your answer as LM5
23Inductors
- V ZI j?LI (NOTE Z j?L)
- In a purely inductive circuit the voltage leads
the current by exactly 90o (or current lags by
90o) - Average power dissipated by an inductor is zero
(stores and releases) ideal - if V 10?50o V, and L2H, ?100 rads/s
- what does I ?
- I V/ j?L V/ j200 10?50o/200?90o
- I 0.05?-40o A
24Impedance (Z) and Reactance (X)
Z V/I
Z R jX
X ?L or X -1/?C
25example problem
- A home in Europe (240VAC/50Hz) that had only
resistive loads (very unlikely) for heating and
lighting converts to a ground-source heat pump (a
motor and compressor) and compact fluorescent
lights. What happens to its current phase angle
if its impedance (Z) prior was 2? resistive and
no reactance and after has 4? of resistance and
10mH of inductance? - V 240?0o V, Z 2?0o ? so I 120?0o A
- V 240?0o V, Z 4 j(314)0.01 5.09?38o ?
- so I V/Z 240?0o/ 5.09?38o 47.2?-38o A
26Memory aid
- ELI the ICE man
- For an inductor (L)
- E (voltage as in EMF) leads current (I)
- same as Current Lags the Voltage
- For a capacitor (C)
- I (the current) leads E (voltage)
- same as Voltage Lags the Current
27R, L C in AC circuits
- SUMMARY
- Currents flowing through any of these elements
(R, L C) will have same frequency as the
voltage supplied by the source - Phase angle shift may result in current depending
on whether there is net L or C in the circuit - Resistive elements are the only circuit
components that dissipate any real energy
28Power factor
- Typical residential and small commercial
watt-hour meters measure only average power,
watts, also called real power. - Utilities must generate power at the power
sources to cover all the demands for current both
real and reactive. - The power factor is a measure of what part of the
overall power in the system is real
29Power factor
- Typically, average power, watts, also called real
power is represented by the following equation - Pavg VI cos? VI x Power Factor
- Where ? is the phase angle (time shift) between V
and I - Therefore, the power factor is identical to
- cos ?
- PF cos ?
30(a) The impedance triangle where Z R jX
(b) The complex power triangle where S P jQ
complex power
31complex impedance (Z) triangle
j?L
Power factor phase angle
1/j?C -j/?C
32power factor
- since cosine function is even with respect to
positive or negative phase angles - i.e cos 45o cos -45o
- we resolve difficulty by labeling power factor
as either leading or lagging - If ?V - ?I gt 0 ? pf is lagging
- If ?V - ?I lt 0 ? pf is leading
- NOTE If pf is leading or lagging THEN the
current (I) is leading or lagging w.r.t. voltage
(V) too!
33Resistive and Reactive Loads
34power factor
- power factor leading or lagging
- lagging with inductive loads/circuit
- leading with capacitive loads/circuit
- utilities generally experience lagging power
factor due to highly inductive loads of
customers - motors, flourescent lights, monitors, tvs,
appliances, dimmer switches, a/c - power factor correction is big part of utility
planning activities
35complex power triangle
? ?S? apparent power
Q reactive power
P real power
36complex power triangle
note ? ?V - ?I
?S? apparent
j
units Volt-Amps
Q reactive
units VARs
P real
units Watts
37Express S,P Q with rms values for V and I LM6
note ? ?V - ?I
?S? apparent
j
units Volt-Amps
Q reactive
units VARs
P real
units Watts
38Power factor example
- A 240-V induction motor draws 30 amps of current
and delivers 5.4kW of power to the shaft, show
its power triangle - Real (average) power 5,400 Watts
- Apparent power (240)(30) 7,200 Volt-Amps
- PF Real/Apparent 5.4kW/7.2kW 0.75
- Phase angle cos-1(0.75) 41.41o
- Draw power triangle and compute reactive power as
LM7 on blank area next to todays work
39Power factor correction?
Why correct power factor? 1/5th of all grid
losses may be due to poor power factor (gt2B/yr),
the outage of 2003 was made more severe by
extremely high reactive demand, all transformers
are rated on kVA not watts, all these economic,
efficiency and reliability benefits can be
achieved at a very low cost
40Power factor correction
Adding capacitive impedance in parallel with the
load enables the current to oscillate between the
inductors and capacitors rather than being drawn
from the utility system or the customer
transformer. Capacitors are rated by
volt-amps-reactive VARs that they supply at the
system voltage in which they are installed, and
PF correction is a straightforward engineering
design
41Power factor correction example
- An industrial customers service entrance
substation is rated at 1MVA (1,000kVA) and is at
95 capacity. The plant now experiences a power
factor of 80. A new manufacturing line is
planned that will increase power demand 125kW.
How many kVAR of capacitance should be added to
avoid purchasing additional substation
transformer capacity? - Real power (at present) (0.8)(0.95)(1,000kVA)
760kW - Phase angle cos-1(0.8) 36.87o
- Apparent power (1,000)(0.95) 9,500 Volt-Amps
- If demand grows from 760kW to 885kW Apparent
Power will grow to Real/PF 885/(0.8) 1106kVA
gt 1MVA capacity - Reactive Power Q VI sin ? 1106(0.6) 664kVAR
42PF correction example (cont)
- An industrial customers service entrance
substation is rated at 1MVA (1,000kVA) and is at
95 capacity. The plant now experiences a power
factor of 80. A new manufacturing line is
planned that will increase power demand 125kW.
How many kVAR of capacitance should be added to
avoid purchasing additional substation
transformer capacity? - For substation to handle the growth, power factor
must improve to at least PF 885kW/1,000kVA
0.885 - Phase angle now will be cos-1(0.885) 27.75o
- Reactive Power (Q) VI sin? 1000(0.4656) 466
kVAR - Difference in reactive power must be supplied by
the capacitor bank 664 466 198 kVAR - Specify a gt 200 kVAR cap bank at industrial
customers service entrance switchgear
433-wire single phase residential wiring
- Figure 2.11 page 68 is helpful
- Figure 2.12 is not as clear
- Panel box is best
443-phase systems
- Benefits
- Generators and motors work more efficiently in
torque transfer and have higher stability (they
run smoother and have less vibration) - Transmission benefits include the reduction
and/or cancellation of neutral return currents so
that less wires and/or smaller common neutrals
can be used.
45 463? current
473? neutral current
48New homework
- HW 2 due next Monday
- will be posted on web
- 2.1, 2.2, 2.3, 2.6, 2.7, 2.8, 2.10