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SG Phasor Diagram and Model Parameter Measurement

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Synchronous Generator
Phasor Diagram
Phasor Diagram
𝐄0
πœ“
𝜹
𝜽
𝐈
𝐄0 = 𝐔 + π‘…π‘Ž 𝐈 + 𝑗𝑋𝑠 𝐈
𝑗𝑋𝑠 𝐈
𝐔
π‘…π‘Ž 𝐈
Definitions:
(Outer) Power Factor Angle 𝜽
οΌˆε€–οΌ‰εŠŸηŽ‡ε› ζ•°θ§’
Inner Power Factor Angle πœ“
ε†…εŠŸηŽ‡ε› ζ•°θ§’
Power Angle
εŠŸοΌˆηŽ‡οΌ‰θ§’
𝜹
Generator Phasor Diagram –
Lagging Power Factor Load
𝐄0
πœ“
𝜹
𝜽
𝐈
𝑗𝑋𝑠 𝐈
𝐔
π‘…π‘Ž 𝐈
𝐄0 = 𝐔 + π‘…π‘Ž 𝐈 + 𝑗𝑋𝑠 𝐈
Over excited (𝐸0 > π‘ˆ)
θΏ‡εŠ±
Generator Phasor Diagram –
Unity Power Factor Load
𝐄0
πœ“
𝐈
𝜽=𝟎
𝜹
𝑗𝑋𝑠 𝐈
𝐔
π‘…π‘Ž 𝐈
𝐄0 = 𝐔 + π‘…π‘Ž 𝐈 + 𝑗𝑋𝑠 𝐈
Slightly over excited (𝐸0 > π‘ˆ)
Generator Phasor Diagram –
Leading Power Factor Load
𝐄0
πœ“ 𝜽
𝑗𝑋𝑠 𝐈
𝐈
𝜹
𝐔
π‘…π‘Ž 𝐈
𝐄0 = 𝐔 + π‘…π‘Ž 𝐈 + 𝑗𝑋𝑠 𝐈
Maybe under excited (𝐸0 < π‘ˆ)
ε―θƒ½ζ¬ εŠ±
Generator Power Flow
(or π‘ƒπ‘’π‘š )
w
π‘‡π‘’π‘š = π‘˜π΅π‘“ 𝐡𝑆 sin 𝛼
π‘ƒπ‘’π‘š = π‘‡π‘’π‘š πœ”π‘š = 3𝐸0 𝐼 cos πœ“
πœ‹
πœ“ = ∠𝐄0 − ∠𝐈 πœ“ = 𝛼 −
2
𝐔 = 𝐄0 − π‘…π‘Ž 𝐈 − 𝑗𝑋𝑠 𝐈
Output Power (1)
𝐄0 = 𝐔 + π‘…π‘Ž 𝐈 + 𝑗𝑋𝑠 𝐈 ≈ 𝐔 + 𝑗𝑋𝑠 𝐈, since π‘…π‘Ž << 𝑋𝑠
π‘ƒπ‘œπ‘’π‘‘ = 3π‘ˆπΌ cos πœƒ
𝐄0
𝑗𝑋𝑠 𝐈 𝜽
πœ“
𝜹
𝐔
𝑋𝑠 𝐼 cos πœƒ
= 𝐸0 sin 𝛿
𝜽
𝐈
π‘ˆ cos πœƒ
= 𝐸0 cos πœ“
π‘ƒπ‘’π‘š ≈ π‘ƒπ‘œπ‘’π‘‘
𝐼 cos πœƒ
𝐸0 sin 𝛿
=
𝑋𝑠
3π‘ˆπΈ0 sin 𝛿
= 3π‘ˆπΌ cos πœƒ =
𝑋𝑆
Output Power (2)
𝐄0 = 𝐔 + π‘…π‘Ž 𝐈 + 𝑗𝑋𝑠 𝐈 ≈ 𝐔 + 𝑗𝑋𝑠 𝐈, since π‘…π‘Ž << 𝑋𝑠
𝐈
πœ“ 𝜽
𝑗𝑋𝑠 𝐈
𝐄0
𝜹
𝐔
𝛼
−𝑗𝑋𝑠 𝐈
𝐄0 − 𝑗𝑋𝑠 𝐈 ≈ 𝐔
𝐁𝑓 + 𝐁𝑠 = 𝐁𝑛𝑒𝑑
欠励(𝐸0 < π‘ˆ), capacitive
πœ‹
𝛼 = ∠𝐄0 − ∠ −𝑗𝑋𝑠 𝐈 = πœ“ +
2
Induced ElectromagneticTorque
π‘ƒπ‘’π‘š
3π‘ˆπΈ0 sin 𝛿
=
= π‘‡π‘’π‘š πœ”π‘š
𝑋𝑆
π‘‡π‘’π‘š
3π‘ˆπΈ0 sin 𝛿
=
πœ”π‘š 𝑋𝑆
π‘‡π‘’π‘š = π‘˜π΅π‘›π‘’π‘‘ 𝐡𝑓 sin 𝛿
Measurement of SG
Model Parameters
Measurement of Model Parameters
1. The relationship between field current If and E0
2. The synchronous reactance XS
3. The armature resistance Ra
Open Circuit Characteristics (OCC)
𝐼=0
𝐸0
ΰ·‘π‘Ž 𝑁
ෑ𝑓
𝐷𝑙 𝑁
𝐸0 = 8 2𝑓𝑒 πœ‡0
𝐼𝑓
𝑔𝑒𝑓𝑓 𝑃2
Saturation for large field current
Short Circuit Characteristics (SCC)
𝐄0 = π‘…π‘Ž 𝐈 + 𝑗𝑋𝑠 𝐈
𝐄0
(or IL )
π‘…π‘Ž 𝐈
𝑗𝑋𝑠 𝐈
𝐁𝑓
πœ“≈
πœ‹
2
𝐈=
π‘ˆ=0
𝐼=
πœ‹
𝛼 =πœ“+ ≈πœ‹
2
𝐁𝑛𝑒𝑑
𝐁𝑆
𝐄0
π‘…π‘Ž + 𝑗𝑋𝑠
𝐸0
𝐡𝑓 ≈ 𝐡𝑆
Bnet ο‚» 0
π‘…π‘Ž2 + 𝑋𝑠2
π‘ˆ=0
No saturation
Measurement of Synchronous Reactance
𝐼𝑠𝑐 =
𝐸0
𝐸0
≈
2
2
𝑋𝑠
π‘…π‘Ž + 𝑋𝑠
𝐸0
⇒ 𝑋𝑠 ≈
𝐼𝑠𝑐
(1)
Therefore, an approximate method for determining the synchronous reactance Xs
at a given field current is:
1.
2.
3.
Get the internal voltage E0 from the OCC at that field current.
Get the short-circuit current flow ISC at that field current from the SCC.
Find Xs by applying (1).
Unsaturated Synchronous Reactance
Saturation for
large field current
𝐸0
𝐼𝑠𝑐
X S ,u
No
saturation
Follow equation
𝑋𝑠 ≈
𝐸0
𝐼𝑠𝑐
The unsaturated synchronous reactance Xs,u can be found simply by applying
𝑋𝑠 ≈ 𝐸0 /𝐼𝑠𝑐
at any field current in the linear portion (on the airgap line) of the OCC curve.
Short-Circuit Ratio
Short Circuit Ratio: The ratio of the field current required for the
rated voltage at open circuit to the field current required for the rated
armature current at short circuit.
𝑆𝐢𝑅 =
πΌπ‘“π‘ˆ |rated voltage at OC
𝐼𝑓𝐼 |rated current at SC
𝐸0
π‘ˆπ‘Ÿπ‘Žπ‘‘π‘’π‘‘
πΌπ‘Ÿπ‘Žπ‘‘π‘’π‘‘
πΌπ‘“π‘ˆ
𝐼𝑓𝐼
𝑆𝐢𝑅 =
πΌπ‘“π‘ˆ
𝐼𝑓𝐼
Measurement of Armature Resistance
The armature resistance Ra can be approximately measured by applying a DC voltage
to the windings while the machine is in stationary and measuring the resulting current
flow. Using DC voltage means that the reactance of the windings will be zero during the
measurement process.
This technique is not perfectly accurate, since the AC resistance will be slightly larger
than the DC resistance (as a results of the skin effect at higher frequencies).
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