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| Inifinite Bus: When fe,gen at no load is slightly higher then fe,bus |
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Definition
| PG>0 in that the generator is supplying power to the bus when connected |
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| Inifinite Bus: When fe,gen is slightly lower that fe,bus |
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Definition
| PG<0 in that the generator is consuming power from the bus when connected |
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| Inifinite Bus: Increasing the Govenor Set points |
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Definition
Increases ωm,nl and fe,gen@nl.
This will then in hand increase EA because EA=KΦmagωm,nl. |
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| Inifinite Bus: After the connection between the bus and the gen... |
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Definition
(a)fe,gen@op = fe,bus and ωm drops to ωbus. EA is fixed and PG increases
(b) VT,gen=VT,bus Vφ is fixed.
PG increases because PG=3VφEAsinδ/ Xs
Therefore sinδ increases
[image]
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Term
| Inifinite Bus: Power factor can be corrected to generate positive Qc by |
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Definition
| Adjusting the field current |
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Term
| Inifinite Bus: Constraints on generators |
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Definition
The power PG must remain constant when changing IF
because (1) generator's speed cannot be changed when connected to the bus(fe cannot change)
(2) the power into the generator is constant(Pin=τindωm) τind is controlled by the govenor set point no IF
(3) Implies that IAcosΘ and EAsinδ do not change when adjusting IF |
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Term
| Inifinite Bus: When field current IF... |
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Definition
the magnetic flux φmax increases. This in turn increases EA=Kφmaxωm. IAcosΘ and EAsinδ
Vφ is constant so the angle of jXsIA changes and IAsinΘ increases(higher positive Q)
[image] |
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Term
| Inifinite Bus: Generator Operated by an Infinite Bus |
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Definition
(1) frequency and terminal volatge are controlled by the system to which it is connected.
(2) Govenor set points of the generator controll the real power supplied by the generator to the system
(3) Field current controls the reactive power suppled by the generator |
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Term
| DC Motors: Three ways to control of Speed Control |
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Definition
(1) Adjusting the field resistance RF( adujusting φs)
(2) Adjusting Armature Voltage VA without changing VT
(3) Inserting a resistor in series with armature circuit
KNOW:
ωm=VA/Kφs - RA/K2φs2τind |
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Term
| DC Motors: Speed Control Via Rf at High speed |
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Definition
This is low torque. There is a decrease in Flux and EA( because Ea=Kφsωm).ωmwill increase because IA increases a lot more than φs decreases. After ωm Increases, IA2 will decrease τind until τind= τLoad.
ωm↑ = VA/Kφs↓ - RA/K2(φs2↓) τind
Graoh showing the behavior at High speed (Slope of -φs2)
[image] |
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Term
| DC Motors: Speed Control Via Rf at Medium speed |
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Definition
| ωm will not change because there is an equal change between IA and φs. |
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Term
| DC Motors: Speed Control Via Rf at Low speed |
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Definition
This is high torque. There is a decrease in Flux and EA( because Ea=Kφsωm)but ωmwill decrease( slow down) because IA increases less than φs decreases. After ωm decreases, IA2 will increase τind until τind= τLoad at a slower speed of ωm .
ωm↓ = VA/Kφs↓ - RA/K2(φs2↓) τind
This is the final plot, the top is at high speed , 3/4 the way is middle and about the bottom is low
[image] |
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Term
| DC Motors: Speed Control Via VA |
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Definition
VT is still constant.
IA=(VA-EA)/RA
When IA increases VA increases and when IA decreases EA increases until Tind = Tload
ωm↑ = VA↑/Kφs - RA/K2(φs2) τind
[image] |
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Term
| DC Motors: Speed Control Via RA |
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Definition
ωm↓ = VA/Kφs - RA↑/K2(φs2) τind
At Same Tload = KφsIA, more power wasted
ωm@Tind=0 = fixed
[image] |
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Term
| Transformer( Per-unit Measurement): Finding the base voltage, Current, Impedance and Apperent Power Everywhere |
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Definition
Ibase=Sbase/Vbase Zbase=(Vbase)2/Sbase
Vbase2=Vbase1/a
Ibase2=Ibase1a
Zbase2=Zbase1/(a)2
Sbase1=Sbase2
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Term
| Transformer( Per-unit Measurement): Converting numbers to Per-unit values |
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Definition
Vx,pu=Vx/Vbase1
Same with all other terms |
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Term
| Transformer( Per-unit Measurement): Solving for Power |
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Definition
(1) Find I of the system I = V/(ZTot)
(2) Find the real power P = real( |I|2Z)
(3) Convert back to actual power P=PpuSbase
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Term
| Transformer( Per-unit Measurement): Voltage Regulation |
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Definition
(1) Find I I=V/Z
(2) Solve for Vp in Vp=Vs,pu +Req,puIpu + jXeq,puI
(3)VR = (Vs-Vp)/Vp |
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| Transformer( Per-unit Measurement): Transformer Efficiency |
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Definition
η= Pout/Pin
=Pout/(Pout + Ploss) |
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Term
| Synchronous Generators: Equivalent Circuit for Vφ |
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Definition
VT=Vφ√3 (θ +/- 30o)
+ for ABC sequence - for ACB sequence
Vφ= EA- jXSIA - RAIA
[image] |
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Term
| Synchronous Generators: Torque |
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Definition
T=P/ω = 9.55O/nr where nr is in RPM
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Term
| Synchronous Generators: Power and Torque Equations |
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Definition
Pconv=3EAIAcosγ
<γ = <EA - <IA
Pout=3VφIAcosθ
Qout=3VφIAsinθ
θ= phase of the load
[image]
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Term
| Synchronous Generators:Simplified Equation for Power |
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Definition
Pout=3VφEAsinδ /Xs
=Pmaxsinδ
δ= γ-Θ ( Phase between EA and Vφ)
γ = the phase between EA and IA
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Term
| Synchronous Generators: Static Power Limit |
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Definition
Xs>>>>RA
Static power limit is when δ=90o or sin(δ) = 1
Therefore static power limit is when
Pout=PMax = 3VφEA /XS |
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Term
| Synchronous Generators: Induced Torque |
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Definition
Is equal to KBRxBs
Which is equal to Tind= Pout/ωm
Where Pout = 3VφEAsinδ/ XS |
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| Synchronous Generators: Finding IA |
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Definition
For Y connection IA=IL
For Delta connection IA =√3IL
and we also know that S=√3VTIL*
(I* represents the complex conjugate of I and therefore means it has a -ve phase i.e -30o)
So if we rearrange for IL, we get:
IL=S/√3VT |
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| Synchronous Generators: Finding Internal Voltage(EA) |
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Definition
(1)Solve for IA
(2) Find Vφ (For Y-connection VT/√3. In Delta Vφ=VT)
(3) Sub all values into the EA equation:
EA=Vφ + RAIA + jXSIA |
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Term
| Synchronous Generators: Finding Pin and Pout |
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Definition
Pout=S*PF
PCLA=3IA2RA
PCLF,dc=IFVF
PIN= Pout+PLosses |
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| Synchronous Generators:Applied Torque |
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Definition
(1) Find the RPM usinf nm=120fe/P
(2)Use the Equations TApp=Pin/ωm |
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Term
| Induction Motors: Rotor Slip |
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Definition
nslip=nsync-nm
s(slip)=nslip/nsync |
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Term
| Induction Motors: Equivalent Circuit |
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Definition
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Term
| Induction Motors: Z equivalent |
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Definition
| Zeq=(R1+jX1)+1/(1/RC +1/jXM + 1/(R2/s +jX2)) |
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Term
| Induction Motors: Air-gap Power |
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Definition
PAG=Pin-PSCL-Pcore = 3I22(R2/s)
Where Pin=3•Re(VφI1*)
PSCL=3I12R1
PCore=3EA2/RC |
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Term
| Induction Motors: Converted & Output Power |
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Definition
PAG=PRCL+Pconv
Where Rotor Copper Losses PRCL=s(3I22(R2/s)) = sPAG
Converted Power: PConv=PAG-PRCL = PAG -sPAG =3I22R2((1-s)/s)
Output Power: Pout= PConv-Pf&W&misc |
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Term
| Induction Motors:Induced Torque |
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Definition
Tind_developed(mech)= Pconv/ωm =PAG/ωsync = Tind_Magnetic(elec)
PAG/ωsync= 3I22(R2/s)/ωsync
I2=VTH/√(RTH+R2/s)2 + (XTH+X2)2
sub this into the Torque equation to get:
Tind=(3VTH2R2/s)/ωsync((RTH+R2/s)2 + (XTH+X2)2)
[image]
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Term
| Induction Motors: Load Torque |
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Definition
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Term
| Induction Motors: Thevenin Equivalent Circuit |
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Definition
VTH≈(XM/X1+XM)Vφ
ZTH≈ R1(XM/X1+XM)2 +jX1
[image] |
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Term
| Induction Motors: Starting Torque |
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Definition
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Term
| Single-Phase Induction Motor: |
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Definition
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