# Stator Vibration Characteristic Identification of Turbogenerator among Single and Composite Faults Composed of Static Air-Gap Eccentricity and Rotor Interturn Short Circuit

Authors: Yu-Ling He; Wei-Qi Deng; Bo Peng; Meng-Qiang Ke; Gui-Ji Tang; Shu-Ting Wan; Xiang-Yu Liu
Journal: Shock and Vibration
 (2016)

---

## Abstract

This paper investigates the radial stator vibration characteristics of turbogenerator under the static air-gap eccentricity (SAGE) fault, the rotor interturn short circuit (RISC) fault, and the composite faults (CFs) composed of SAGE and RISC, respectively. Firstly, the impact of the faulty types on the magnetic flux density (MFD) is analyzed, based on which the detailed expressions of the magnetic pull per unit area (MPPUA) on the stator under different performing conditions are deduced. Then, numerical FEM simulations based on Ansoft and an experimental study are carried out, taking the SDF-9 type fault simulating generator as the study object. It is shown that SAGE will increase the stator vibration at 2f (f is the electrical frequency) which already exists even in normal condition, while RISC and CF will bring in stator vibrations atf, 2f, 3f, and 4f at the same time. The vibration amplitudes under CF are larger than those under RISC. As SAGE increases, the vibration amplitudes of each harmonic component under CF will all be increased, while the development of RISC will decrease the 2nd harmonic vibration but meanwhile increase the 4th harmonic vibration. The achievements of this paper are beneficial for fault identification and condition monitoring of the turbogenerator.


---

## Body

## 1. Introduction

SAGE and RISC are common faults of turbogenerator. When the eccentricity degree is more than 10%, severe vibrations, stator core deformations, and even winding damage will be caused [1]. When RISC fault develops progressively, serious consequences, such as field current increment, reactive power output decrease, and bearing vibration aggravation, will be produced. It may also develop into an earth fault and magnetize the rotor. More severely, the shaft journal and the bearing bush may also be burned out [2].By far, scholars have paid much attention to either SAGE or RISC, while few of them studied the CF considering these two faults occurring at the same time. Achievements obtained for SAGE mainly focus on the three-phase current or voltage change [3–6], the circulating current inside parallel branches (CCPB) and its corresponding diagnosis method [7–9], the unbalanced magnetic pull (UMP) calculation via FEM [10, 11], the winding inductance variation based on improved winding function theory [12], and so forth.For RISC, the primary monitor performances are taken by means of installing extra search coils inside the generator [13]. Meanwhile, the detective methods based on the shaft voltage [14, 15] and the CCPB characteristics [16] have also been found as effective tools for this fault. However, the search coil method and the CCPB-based method need to install extra components such as the search coils and the current transformers inside the generator, which is actually not welcomed by the practical performers and needs a higher cost. Relatively, methods based on the stator and rotor vibration characteristics [17, 18] and the electromagnetic torque (EMT) [19] are much more convenient due to the easy accomplishment on vibration and EMT data obtaining. The vibrations can be easily obtained by the velocity and acceleration sensors which have usually been already set up inside the generator or by setting sensors outside the generator conveniently, while the EMT can be calculated by using the phase voltages, currents, and the rotating speed of the rotor which can be easily obtained without installing extra sensors [19].Currently, achievements obtained by scholars have set up a good basis for condition monitoring and diagnosis for these two faults. However, since SAGE exists in almost every generator, there is actually a CF occurring when RISC takes place. Previous studies on this kind of CF found that the failure characteristics are different from those of the single SAGE and RISC faults [20]. Moreover, it has been also found that the rotor vibration has very similar features under many different faults. For example, the mass unbalance of the rotor, the RISC fault, and the stator interturn short circuit (SISC) will all cause rotor vibrations atf [20–22]. However, the stator vibration properties are found to be much more distinguishable. The stator will vibrate atf, 2f, 3f, and 4f under RISC [20, 21] and 2f, 4f, and 6f under SISC [23, 24], respectively, while under the mass unbalance fault the stator vibration will change very little. Therefore, comparably, the stator vibration has a more sensitive effect to identify the failure types, though most scholars have paid their primary attention to the rotor vibrations but not the stator vibration characteristics [18, 20–22, 24].As an improvement, this paper investigates the stator vibration characteristics under SAGE, RISC, and CF composed of SAGE and RISC, respectively, in order to obtain a significant identification criterion for these three faults. The whole work is taken based on the theoretical analysis, the numerical FEM simulation, and the experiment study.


## 2. Theoretical Analysis

### 2.1. Magnetic Flux Density

The air-gap magnetic flux density (MFD) is composed of the magnetomotive force (MMF) and the permeance per unit area (PPUA) through a multiplying operation. Generally, RISC mainly affects MMF, while SAGE primarily affects PPUA. Thus, MFD will be affected by either of these two faults. Typically, the air gap and MMFs under different conditions are indicated in Figure1 [20].Figure 1
Air gap and MMFs of turbogenerator under different conditions.
(a)
Normal (Λ
0
=
μ
0
/
g)
(b)
SAGE (Λ
(
α
m
)
=
μ
0
/
(
g
0
-
δ
s
cos
⁡
α
m
)
=
Λ
0
+
Λ
s
cos
⁡
α
m)
(c)
MMF under normal condition and SAGE
(d)
MMF under RISC and CFPPUAs and MMFs for each case can be written as(1)
Λ
N
o
r
m
a
l
α
m
,
t
=
μ
0
g
0
=
Λ
0
Normal  condition,  RISC
,
Λ
S
G
E
α
m
,
t
=
μ
0
g
α
m
,
t
=
μ
0
g
0
1
-
δ
s
cos
⁡
α
m
≈
Λ
0
1
+
δ
s
cos
⁡
α
m
=
Λ
0
+
Λ
s
cos
⁡
α
m
SAGE,  CF
,
(2)
f
N
o
r
m
a
l
α
m
,
t
=
F
s
cos
⁡
ω
t
-
α
m
-
ψ
-
0.5
π
+
F
r
cos
⁡
ω
t
-
α
m
=
F
1
cos
⁡
ω
t
-
α
m
-
β
Normal  condition,  SAGE
,
f
R
I
S
C
α
m
,
t
=
F
1
cos
⁡
ω
t
-
α
m
-
β
-
F
d
1
cos
⁡
ω
t
-
α
m
-
φ
1
-
F
d
2
cos
⁡
2
ω
t
-
α
m
-
π
-
φ
2
=
F
C
cos
⁡
ω
t
-
α
m
-
β
′
-
F
d
2
cos
⁡
2
ω
t
-
α
m
-
π
-
φ
2
RISC,  CF
,where(3)
F
1
=
F
r
-
F
s
sin
⁡
ψ
2
+
F
s
cos
⁡
ψ
2
,
β
=
arctan
⁡
F
s
cos
⁡
ψ
F
r
-
F
s
sin
⁡
ψ
,
F
C
=
F
r
-
F
s
sin
⁡
ψ
-
F
d
1
cos
⁡
φ
1
2
+
F
s
cos
⁡
ψ
-
F
d
1
sin
⁡
φ
1
2
,
β
′
=
arctan
⁡
F
s
cos
⁡
ψ
-
F
d
1
sin
⁡
φ
1
F
r
-
F
s
sin
⁡
ψ
-
F
d
1
cos
⁡
φ
1
.Correspondingly, MFDs under different conditions are(4a)
B
α
m
,
t
=
F
1
Λ
0
cos
⁡
ω
t
-
α
m
-
β
Normal  condition
,
(4b)
B
α
m
,
t
=
F
1
Λ
0
+
Λ
s
cos
⁡
α
m
cos
⁡
ω
t
-
α
m
-
β
S
A
G
E
,
(4c)
B
α
m
,
t
=
F
C
cos
⁡
ω
t
-
α
m
-
β
′
-
F
d
2
cos
⁡
2
ω
t
-
α
m
-
π
-
φ
2
Λ
0
R
I
S
C
,
(4d)
B
α
m
,
t
=
Λ
0
+
Λ
s
cos
⁡
α
m
F
C
cos
⁡
ω
t
-
α
m
-
β
′
-
Λ
0
+
Λ
s
cos
⁡
α
m
F
d
2
cos
⁡
2
ω
t
-
π
-
α
m
-
φ
2
C
F
,where F
1 and F
C are the composite MMFs of 1st harmonic under normal condition and CF, respectively (F
1
>
F
C). F
r and F
s are, respectively, the rotor MMF and the stator MMF at the fundamental frequency. F
d
1 and F
d
2 are the reverse MMFs of 1st and 2nd harmonic produced by RISC. Λ
0 is the constant component of PPUA, while Λ
s
=
Λ
0
δ
s is the component caused by the SAGE. α
m is a mechanical angle to indicate the circumferential position of the air gap.As indicated in (4a)–(4d), MFDs under normal condition and SAGE are mainly composed of 1st harmonic components, with the amplitudes of F
1
Λ
0 and F
1
(
Λ
0
+
Λ
s
cos
⁡
α
m
), respectively. Actually, the occurrence of SAGE will generally increase the permeance, because the full expansion of the power series (the second formula in (1)) is Λ
0
(
1
+
Λ
s
cos
⁡
α
m
+
0.5
Λ
s
2
+
0.5
cos
⁡
2
α
m
+
⋯
), which is obviously larger than the normal permeance Λ
0. Consequently, as SAGE is increased, the faulty MFD amplitude will be enlarged.However, in the cases of RISC and CF, besides the 1st harmonic components, 2nd harmonic components also exist. As RISC develops, the inverse MMFs of 1st harmonic and 2nd harmonic will both be increased, resulting in the decrease of the 1st MFD but meanwhile the increment of the 2nd MFD (see Figure1(d)).


### 2.2. Exciting Characteristics of MPPUA

#### 2.2.1. Stator Structure and Essential Exciting Force

The generator stator is made up of the stator core, the windings, the frame, the end covers, and so forth. Stator vibrations are primarily produced by the magnetic forces acting on the stator core. This kind of magnetic force is actually a unit magnetic pull performing on the whole inner surface of the stator core, usually called magnetic pull per unit area (MPPUA), as indicated in Figure2. Since the structure of the stator core is similar to a hollow shell, its radial rigidity is small. Even if the resultant force of MPPUA over the whole inner face is zero, the stator core will still have a periodic shrinking-expanding deformation under the excitation of the pulsating MPPUA. Typically, this periodic shrinking-expanding deformation is actually the radial vibration, which has been well known by people.Figure 2
Structure and magnetic force of stator core.
(a)
Structure of stator core
(b)
MPPUA on stator coreMPPUA mainly acts on the stator core surface, and the composite magnetic pulls can be obtained by integrating MPPUA. Because the stator core is a shell structure that is made up of silicon steel sheets, the radial rigidity is small and the composite magnetic pull is zero (shown in Figure2). However, under the periodic MPPUA, the stator core also can generate the radial vibration, such as the periodic expansion-contraction. Therefore, MPPUA is the nature exciting force of stator vibration.Therefore, due to the specific structure of the stator core, the essential exciting force for the stator vibration is MPPUA, which can be deduced based on(5)
q
α
m
,
t
=
B
2
α
m
,
t
2
μ
0
.


#### 2.2.2. Exciting Characteristics of MPPUA

Substituting (4a)–(4d) into (5), the MPPUA expressions, respectively, under normal condition, SAGE, RISC, and CF can be obtained: (6a)
q
α
m
,
t
=
F
1
2
Λ
0
2
4
μ
0
1
+
cos
⁡
2
ω
t
-
2
α
m
-
2
β
N
o
r
m
a
l
c
o
n
d
i
t
i
o
n
,
(6b)
q
α
m
,
t
=
F
1
2
8
μ
0
2
Λ
0
2
+
Λ
s
2
+
4
Λ
0
Λ
s
cos
⁡
α
m
+
Λ
s
2
cos
⁡
2
α
m
+
0.5
Λ
s
2
cos
⁡
2
ω
t
-
2
β
+
2
Λ
0
Λ
s
cos
⁡
2
ω
t
-
α
m
-
2
β
+
2
Λ
0
2
+
Λ
s
2
cos
⁡
2
ω
t
-
2
α
m
-
2
β
+
2
Λ
0
Λ
s
cos
⁡
2
ω
t
-
3
α
m
-
2
β
+
0.5
Λ
s
2
cos
⁡
2
ω
t
-
4
α
m
-
2
β
S
A
G
E
,
(6c)
q
α
m
,
t
=
Λ
0
2
4
μ
0
F
C
2
+
F
d
2
2
-
2
F
C
F
d
2
cos
⁡
ω
t
-
α
m
+
β
1
-
2
φ
2
+
F
C
2
cos
⁡
2
ω
t
-
α
m
-
β
-
2
F
C
F
d
2
cos
⁡
3
ω
t
-
3
α
m
-
β
1
-
2
φ
2
+
F
d
2
2
cos
⁡
4
ω
t
-
α
m
-
φ
2
R
I
S
C
,
(6d)
q
α
m
,
t
=
1
8
μ
0
F
C
2
+
F
d
2
2
2
Λ
0
2
+
Λ
s
2
+
4
F
C
2
+
F
d
2
2
Λ
0
Λ
s
cos
⁡
α
m
+
F
C
2
+
F
d
2
2
Λ
s
2
cos
⁡
2
α
m
+
F
C
F
d
2
-
4
Λ
0
Λ
s
cos
⁡
ω
t
+
β
1
-
2
φ
2
-
2
2
Λ
0
2
+
Λ
s
2
cos
⁡
ω
t
-
α
m
+
β
1
-
2
φ
2
-
Λ
s
2
cos
⁡
ω
t
+
α
m
+
β
1
-
2
φ
2
-
4
Λ
0
Λ
s
cos
⁡
ω
t
-
2
α
m
+
β
1
-
2
φ
2
-
Λ
s
2
cos
⁡
ω
t
-
3
α
m
+
β
1
-
2
φ
2
+
F
C
2
0.5
Λ
s
2
cos
⁡
2
ω
t
-
2
β
1
+
2
Λ
0
Λ
s
cos
⁡
2
ω
t
-
α
m
-
2
β
1
+
2
Λ
0
2
+
Λ
s
2
cos
⁡
2
ω
t
-
2
α
m
-
2
β
1
+
2
Λ
0
Λ
s
cos
⁡
2
ω
t
-
3
α
m
-
2
β
1
+
0.5
Λ
s
2
cos
⁡
2
ω
t
-
4
α
m
-
2
β
1
+
F
C
F
d
2
-
Λ
s
2
cos
⁡
3
ω
t
-
α
m
-
β
1
-
2
φ
2
-
4
Λ
0
Λ
s
cos
⁡
3
ω
t
-
2
α
m
-
β
1
-
2
φ
2
-
2
2
Λ
0
2
+
Λ
s
2
cos
⁡
3
ω
t
-
3
α
m
-
β
1
-
2
φ
2
-
4
Λ
0
Λ
s
cos
⁡
3
ω
t
-
4
α
m
-
β
1
-
2
φ
2
-
Λ
s
2
cos
⁡
3
ω
t
-
5
α
m
-
β
1
-
2
φ
2
+
F
d
2
2
0.5
Λ
s
2
cos
⁡
4
ω
t
-
2
α
m
-
4
φ
2
+
2
Λ
0
Λ
s
cos
⁡
4
ω
t
-
3
α
m
-
4
φ
2
+
2
Λ
0
2
+
Λ
s
2
cos
⁡
4
ω
t
-
4
α
m
-
4
φ
2
+
2
Λ
0
Λ
s
cos
⁡
4
ω
t
-
5
α
m
-
4
φ
2
+
0.5
Λ
s
2
cos
⁡
4
ω
t
-
6
α
m
-
4
φ
2
C
F
.As indicated in (6a)–(6d), MPPUA has different pulsating components under different performing conditions. Since the stator vibration is actually the response of the exciting MPPUA, the vibration spectrum should have the same harmonic components as MPPUA. Obviously, under normal condition and SAGE, the stator vibration has only 2nd harmonic components (the DC component force will not bring in vibrations to the stator but will induce a radial deformation tendency after a long action). The occurrence of SAGE will increase the vibration amplitude at 2f. However, when RISC or CF takes place, besides the 2nd harmonic components, 1st, 3rd, and 4th harmonic components will also be produced. To further study the exciting characteristics of MPPUA and the stator vibration response features, the upper amplitude expressions of each MPPUA component under different conditions are shown in Table 1, where I
f is the exciting current of the generator, f
s
d is the shorted degree of RISC, and δ
s is the relative SAGE value.Table 1
Upper amplitude expressions of MPPUA for different conditions.
Component
Performing condition
Amplitude formulas
Influential factors
DC component
Normal condition
F
1
2
Λ
0
2
/
4
μ
0
I
f
SAGE
F
1
2
Λ
0
+
Λ
s
2
/
4
μ
0
I
f, δ
s
RISC
(
F
C
2
+
F
d
2
2
)
Λ
0
2
/
4
μ
0
I
f, f
s
d
CF
(
F
C
2
+
F
d
2
2
)
Λ
0
+
Λ
s
2
/
4
μ
0
I
f, δ
s, f
s
d
1st harmonic
Normal condition
—
—
SAGE
—
—
RISC
-
F
C
F
d
2
Λ
0
2
/
2
μ
0
I
f, f
s
d
CF
F
C
F
d
2
Λ
0
+
Λ
s
2
/
2
μ
0
I
f, δ
s, f
s
d
2nd harmonic
Normal condition
F
1
2
Λ
0
2
/
4
μ
0
I
f
SAGE
F
1
2
Λ
0
+
Λ
s
2
/
4
μ
0
I
f, δ
s
RISC
F
C
2
Λ
0
2
/
4
μ
0
I
f, f
s
d
CF
F
C
2
Λ
0
+
Λ
s
2
/
4
μ
0
I
f, δ
s, f
s
d
3rd harmonic
Normal condition
—
—
SAGE
—
—
RISC
-
F
C
F
d
2
Λ
0
2
/
2
μ
0
I
f, f
s
d
CF
F
C
F
d
2
Λ
0
+
Λ
s
2
/
2
μ
0
I
f, δ
s, f
s
d
4th harmonic
Normal condition
—
—
SAGE
—
—
RISC
F
d
2
2
Λ
0
2
/
4
μ
0
I
f, f
s
d
CF
F
d
2
2
Λ
0
+
Λ
s
2
/
4
μ
0
I
f, δ
s, f
s
dAs shown in Table1, SAGE has larger MPPUA magnitude at 2f, while RISC has smaller MPPUA magnitude at 2f than normal condition. Specifically, CF has larger MPPUA amplitudes atf, 2f, 3f, and 4f than RISC. Consequently, the occurrence of SAGE will increase the 2nd harmonic vibration of stator, while RISC will decrease the 2nd harmonic vibration amplitude. The stator vibration amplitudes atf, 2f, 3f, and 4f under CF condition will be more intense than under RISC condition. This can be used for the fault identification among the single and the composite faults composed of SAGE and RISC.


## 2.1. Magnetic Flux Density

The air-gap magnetic flux density (MFD) is composed of the magnetomotive force (MMF) and the permeance per unit area (PPUA) through a multiplying operation. Generally, RISC mainly affects MMF, while SAGE primarily affects PPUA. Thus, MFD will be affected by either of these two faults. Typically, the air gap and MMFs under different conditions are indicated in Figure1 [20].Figure 1
Air gap and MMFs of turbogenerator under different conditions.
(a)
Normal (Λ
0
=
μ
0
/
g)
(b)
SAGE (Λ
(
α
m
)
=
μ
0
/
(
g
0
-
δ
s
cos
⁡
α
m
)
=
Λ
0
+
Λ
s
cos
⁡
α
m)
(c)
MMF under normal condition and SAGE
(d)
MMF under RISC and CFPPUAs and MMFs for each case can be written as(1)
Λ
N
o
r
m
a
l
α
m
,
t
=
μ
0
g
0
=
Λ
0
Normal  condition,  RISC
,
Λ
S
G
E
α
m
,
t
=
μ
0
g
α
m
,
t
=
μ
0
g
0
1
-
δ
s
cos
⁡
α
m
≈
Λ
0
1
+
δ
s
cos
⁡
α
m
=
Λ
0
+
Λ
s
cos
⁡
α
m
SAGE,  CF
,
(2)
f
N
o
r
m
a
l
α
m
,
t
=
F
s
cos
⁡
ω
t
-
α
m
-
ψ
-
0.5
π
+
F
r
cos
⁡
ω
t
-
α
m
=
F
1
cos
⁡
ω
t
-
α
m
-
β
Normal  condition,  SAGE
,
f
R
I
S
C
α
m
,
t
=
F
1
cos
⁡
ω
t
-
α
m
-
β
-
F
d
1
cos
⁡
ω
t
-
α
m
-
φ
1
-
F
d
2
cos
⁡
2
ω
t
-
α
m
-
π
-
φ
2
=
F
C
cos
⁡
ω
t
-
α
m
-
β
′
-
F
d
2
cos
⁡
2
ω
t
-
α
m
-
π
-
φ
2
RISC,  CF
,where(3)
F
1
=
F
r
-
F
s
sin
⁡
ψ
2
+
F
s
cos
⁡
ψ
2
,
β
=
arctan
⁡
F
s
cos
⁡
ψ
F
r
-
F
s
sin
⁡
ψ
,
F
C
=
F
r
-
F
s
sin
⁡
ψ
-
F
d
1
cos
⁡
φ
1
2
+
F
s
cos
⁡
ψ
-
F
d
1
sin
⁡
φ
1
2
,
β
′
=
arctan
⁡
F
s
cos
⁡
ψ
-
F
d
1
sin
⁡
φ
1
F
r
-
F
s
sin
⁡
ψ
-
F
d
1
cos
⁡
φ
1
.Correspondingly, MFDs under different conditions are(4a)
B
α
m
,
t
=
F
1
Λ
0
cos
⁡
ω
t
-
α
m
-
β
Normal  condition
,
(4b)
B
α
m
,
t
=
F
1
Λ
0
+
Λ
s
cos
⁡
α
m
cos
⁡
ω
t
-
α
m
-
β
S
A
G
E
,
(4c)
B
α
m
,
t
=
F
C
cos
⁡
ω
t
-
α
m
-
β
′
-
F
d
2
cos
⁡
2
ω
t
-
α
m
-
π
-
φ
2
Λ
0
R
I
S
C
,
(4d)
B
α
m
,
t
=
Λ
0
+
Λ
s
cos
⁡
α
m
F
C
cos
⁡
ω
t
-
α
m
-
β
′
-
Λ
0
+
Λ
s
cos
⁡
α
m
F
d
2
cos
⁡
2
ω
t
-
π
-
α
m
-
φ
2
C
F
,where F
1 and F
C are the composite MMFs of 1st harmonic under normal condition and CF, respectively (F
1
>
F
C). F
r and F
s are, respectively, the rotor MMF and the stator MMF at the fundamental frequency. F
d
1 and F
d
2 are the reverse MMFs of 1st and 2nd harmonic produced by RISC. Λ
0 is the constant component of PPUA, while Λ
s
=
Λ
0
δ
s is the component caused by the SAGE. α
m is a mechanical angle to indicate the circumferential position of the air gap.As indicated in (4a)–(4d), MFDs under normal condition and SAGE are mainly composed of 1st harmonic components, with the amplitudes of F
1
Λ
0 and F
1
(
Λ
0
+
Λ
s
cos
⁡
α
m
), respectively. Actually, the occurrence of SAGE will generally increase the permeance, because the full expansion of the power series (the second formula in (1)) is Λ
0
(
1
+
Λ
s
cos
⁡
α
m
+
0.5
Λ
s
2
+
0.5
cos
⁡
2
α
m
+
⋯
), which is obviously larger than the normal permeance Λ
0. Consequently, as SAGE is increased, the faulty MFD amplitude will be enlarged.However, in the cases of RISC and CF, besides the 1st harmonic components, 2nd harmonic components also exist. As RISC develops, the inverse MMFs of 1st harmonic and 2nd harmonic will both be increased, resulting in the decrease of the 1st MFD but meanwhile the increment of the 2nd MFD (see Figure1(d)).


## 2.2. Exciting Characteristics of MPPUA

### 2.2.1. Stator Structure and Essential Exciting Force

The generator stator is made up of the stator core, the windings, the frame, the end covers, and so forth. Stator vibrations are primarily produced by the magnetic forces acting on the stator core. This kind of magnetic force is actually a unit magnetic pull performing on the whole inner surface of the stator core, usually called magnetic pull per unit area (MPPUA), as indicated in Figure2. Since the structure of the stator core is similar to a hollow shell, its radial rigidity is small. Even if the resultant force of MPPUA over the whole inner face is zero, the stator core will still have a periodic shrinking-expanding deformation under the excitation of the pulsating MPPUA. Typically, this periodic shrinking-expanding deformation is actually the radial vibration, which has been well known by people.Figure 2
Structure and magnetic force of stator core.
(a)
Structure of stator core
(b)
MPPUA on stator coreMPPUA mainly acts on the stator core surface, and the composite magnetic pulls can be obtained by integrating MPPUA. Because the stator core is a shell structure that is made up of silicon steel sheets, the radial rigidity is small and the composite magnetic pull is zero (shown in Figure2). However, under the periodic MPPUA, the stator core also can generate the radial vibration, such as the periodic expansion-contraction. Therefore, MPPUA is the nature exciting force of stator vibration.Therefore, due to the specific structure of the stator core, the essential exciting force for the stator vibration is MPPUA, which can be deduced based on(5)
q
α
m
,
t
=
B
2
α
m
,
t
2
μ
0
.


### 2.2.2. Exciting Characteristics of MPPUA

Substituting (4a)–(4d) into (5), the MPPUA expressions, respectively, under normal condition, SAGE, RISC, and CF can be obtained: (6a)
q
α
m
,
t
=
F
1
2
Λ
0
2
4
μ
0
1
+
cos
⁡
2
ω
t
-
2
α
m
-
2
β
N
o
r
m
a
l
c
o
n
d
i
t
i
o
n
,
(6b)
q
α
m
,
t
=
F
1
2
8
μ
0
2
Λ
0
2
+
Λ
s
2
+
4
Λ
0
Λ
s
cos
⁡
α
m
+
Λ
s
2
cos
⁡
2
α
m
+
0.5
Λ
s
2
cos
⁡
2
ω
t
-
2
β
+
2
Λ
0
Λ
s
cos
⁡
2
ω
t
-
α
m
-
2
β
+
2
Λ
0
2
+
Λ
s
2
cos
⁡
2
ω
t
-
2
α
m
-
2
β
+
2
Λ
0
Λ
s
cos
⁡
2
ω
t
-
3
α
m
-
2
β
+
0.5
Λ
s
2
cos
⁡
2
ω
t
-
4
α
m
-
2
β
S
A
G
E
,
(6c)
q
α
m
,
t
=
Λ
0
2
4
μ
0
F
C
2
+
F
d
2
2
-
2
F
C
F
d
2
cos
⁡
ω
t
-
α
m
+
β
1
-
2
φ
2
+
F
C
2
cos
⁡
2
ω
t
-
α
m
-
β
-
2
F
C
F
d
2
cos
⁡
3
ω
t
-
3
α
m
-
β
1
-
2
φ
2
+
F
d
2
2
cos
⁡
4
ω
t
-
α
m
-
φ
2
R
I
S
C
,
(6d)
q
α
m
,
t
=
1
8
μ
0
F
C
2
+
F
d
2
2
2
Λ
0
2
+
Λ
s
2
+
4
F
C
2
+
F
d
2
2
Λ
0
Λ
s
cos
⁡
α
m
+
F
C
2
+
F
d
2
2
Λ
s
2
cos
⁡
2
α
m
+
F
C
F
d
2
-
4
Λ
0
Λ
s
cos
⁡
ω
t
+
β
1
-
2
φ
2
-
2
2
Λ
0
2
+
Λ
s
2
cos
⁡
ω
t
-
α
m
+
β
1
-
2
φ
2
-
Λ
s
2
cos
⁡
ω
t
+
α
m
+
β
1
-
2
φ
2
-
4
Λ
0
Λ
s
cos
⁡
ω
t
-
2
α
m
+
β
1
-
2
φ
2
-
Λ
s
2
cos
⁡
ω
t
-
3
α
m
+
β
1
-
2
φ
2
+
F
C
2
0.5
Λ
s
2
cos
⁡
2
ω
t
-
2
β
1
+
2
Λ
0
Λ
s
cos
⁡
2
ω
t
-
α
m
-
2
β
1
+
2
Λ
0
2
+
Λ
s
2
cos
⁡
2
ω
t
-
2
α
m
-
2
β
1
+
2
Λ
0
Λ
s
cos
⁡
2
ω
t
-
3
α
m
-
2
β
1
+
0.5
Λ
s
2
cos
⁡
2
ω
t
-
4
α
m
-
2
β
1
+
F
C
F
d
2
-
Λ
s
2
cos
⁡
3
ω
t
-
α
m
-
β
1
-
2
φ
2
-
4
Λ
0
Λ
s
cos
⁡
3
ω
t
-
2
α
m
-
β
1
-
2
φ
2
-
2
2
Λ
0
2
+
Λ
s
2
cos
⁡
3
ω
t
-
3
α
m
-
β
1
-
2
φ
2
-
4
Λ
0
Λ
s
cos
⁡
3
ω
t
-
4
α
m
-
β
1
-
2
φ
2
-
Λ
s
2
cos
⁡
3
ω
t
-
5
α
m
-
β
1
-
2
φ
2
+
F
d
2
2
0.5
Λ
s
2
cos
⁡
4
ω
t
-
2
α
m
-
4
φ
2
+
2
Λ
0
Λ
s
cos
⁡
4
ω
t
-
3
α
m
-
4
φ
2
+
2
Λ
0
2
+
Λ
s
2
cos
⁡
4
ω
t
-
4
α
m
-
4
φ
2
+
2
Λ
0
Λ
s
cos
⁡
4
ω
t
-
5
α
m
-
4
φ
2
+
0.5
Λ
s
2
cos
⁡
4
ω
t
-
6
α
m
-
4
φ
2
C
F
.As indicated in (6a)–(6d), MPPUA has different pulsating components under different performing conditions. Since the stator vibration is actually the response of the exciting MPPUA, the vibration spectrum should have the same harmonic components as MPPUA. Obviously, under normal condition and SAGE, the stator vibration has only 2nd harmonic components (the DC component force will not bring in vibrations to the stator but will induce a radial deformation tendency after a long action). The occurrence of SAGE will increase the vibration amplitude at 2f. However, when RISC or CF takes place, besides the 2nd harmonic components, 1st, 3rd, and 4th harmonic components will also be produced. To further study the exciting characteristics of MPPUA and the stator vibration response features, the upper amplitude expressions of each MPPUA component under different conditions are shown in Table 1, where I
f is the exciting current of the generator, f
s
d is the shorted degree of RISC, and δ
s is the relative SAGE value.Table 1
Upper amplitude expressions of MPPUA for different conditions.
Component
Performing condition
Amplitude formulas
Influential factors
DC component
Normal condition
F
1
2
Λ
0
2
/
4
μ
0
I
f
SAGE
F
1
2
Λ
0
+
Λ
s
2
/
4
μ
0
I
f, δ
s
RISC
(
F
C
2
+
F
d
2
2
)
Λ
0
2
/
4
μ
0
I
f, f
s
d
CF
(
F
C
2
+
F
d
2
2
)
Λ
0
+
Λ
s
2
/
4
μ
0
I
f, δ
s, f
s
d
1st harmonic
Normal condition
—
—
SAGE
—
—
RISC
-
F
C
F
d
2
Λ
0
2
/
2
μ
0
I
f, f
s
d
CF
F
C
F
d
2
Λ
0
+
Λ
s
2
/
2
μ
0
I
f, δ
s, f
s
d
2nd harmonic
Normal condition
F
1
2
Λ
0
2
/
4
μ
0
I
f
SAGE
F
1
2
Λ
0
+
Λ
s
2
/
4
μ
0
I
f, δ
s
RISC
F
C
2
Λ
0
2
/
4
μ
0
I
f, f
s
d
CF
F
C
2
Λ
0
+
Λ
s
2
/
4
μ
0
I
f, δ
s, f
s
d
3rd harmonic
Normal condition
—
—
SAGE
—
—
RISC
-
F
C
F
d
2
Λ
0
2
/
2
μ
0
I
f, f
s
d
CF
F
C
F
d
2
Λ
0
+
Λ
s
2
/
2
μ
0
I
f, δ
s, f
s
d
4th harmonic
Normal condition
—
—
SAGE
—
—
RISC
F
d
2
2
Λ
0
2
/
4
μ
0
I
f, f
s
d
CF
F
d
2
2
Λ
0
+
Λ
s
2
/
4
μ
0
I
f, δ
s, f
s
dAs shown in Table1, SAGE has larger MPPUA magnitude at 2f, while RISC has smaller MPPUA magnitude at 2f than normal condition. Specifically, CF has larger MPPUA amplitudes atf, 2f, 3f, and 4f than RISC. Consequently, the occurrence of SAGE will increase the 2nd harmonic vibration of stator, while RISC will decrease the 2nd harmonic vibration amplitude. The stator vibration amplitudes atf, 2f, 3f, and 4f under CF condition will be more intense than under RISC condition. This can be used for the fault identification among the single and the composite faults composed of SAGE and RISC.


## 2.2.1. Stator Structure and Essential Exciting Force

The generator stator is made up of the stator core, the windings, the frame, the end covers, and so forth. Stator vibrations are primarily produced by the magnetic forces acting on the stator core. This kind of magnetic force is actually a unit magnetic pull performing on the whole inner surface of the stator core, usually called magnetic pull per unit area (MPPUA), as indicated in Figure2. Since the structure of the stator core is similar to a hollow shell, its radial rigidity is small. Even if the resultant force of MPPUA over the whole inner face is zero, the stator core will still have a periodic shrinking-expanding deformation under the excitation of the pulsating MPPUA. Typically, this periodic shrinking-expanding deformation is actually the radial vibration, which has been well known by people.Figure 2
Structure and magnetic force of stator core.
(a)
Structure of stator core
(b)
MPPUA on stator coreMPPUA mainly acts on the stator core surface, and the composite magnetic pulls can be obtained by integrating MPPUA. Because the stator core is a shell structure that is made up of silicon steel sheets, the radial rigidity is small and the composite magnetic pull is zero (shown in Figure2). However, under the periodic MPPUA, the stator core also can generate the radial vibration, such as the periodic expansion-contraction. Therefore, MPPUA is the nature exciting force of stator vibration.Therefore, due to the specific structure of the stator core, the essential exciting force for the stator vibration is MPPUA, which can be deduced based on(5)
q
α
m
,
t
=
B
2
α
m
,
t
2
μ
0
.


## 2.2.2. Exciting Characteristics of MPPUA

Substituting (4a)–(4d) into (5), the MPPUA expressions, respectively, under normal condition, SAGE, RISC, and CF can be obtained: (6a)
q
α
m
,
t
=
F
1
2
Λ
0
2
4
μ
0
1
+
cos
⁡
2
ω
t
-
2
α
m
-
2
β
N
o
r
m
a
l
c
o
n
d
i
t
i
o
n
,
(6b)
q
α
m
,
t
=
F
1
2
8
μ
0
2
Λ
0
2
+
Λ
s
2
+
4
Λ
0
Λ
s
cos
⁡
α
m
+
Λ
s
2
cos
⁡
2
α
m
+
0.5
Λ
s
2
cos
⁡
2
ω
t
-
2
β
+
2
Λ
0
Λ
s
cos
⁡
2
ω
t
-
α
m
-
2
β
+
2
Λ
0
2
+
Λ
s
2
cos
⁡
2
ω
t
-
2
α
m
-
2
β
+
2
Λ
0
Λ
s
cos
⁡
2
ω
t
-
3
α
m
-
2
β
+
0.5
Λ
s
2
cos
⁡
2
ω
t
-
4
α
m
-
2
β
S
A
G
E
,
(6c)
q
α
m
,
t
=
Λ
0
2
4
μ
0
F
C
2
+
F
d
2
2
-
2
F
C
F
d
2
cos
⁡
ω
t
-
α
m
+
β
1
-
2
φ
2
+
F
C
2
cos
⁡
2
ω
t
-
α
m
-
β
-
2
F
C
F
d
2
cos
⁡
3
ω
t
-
3
α
m
-
β
1
-
2
φ
2
+
F
d
2
2
cos
⁡
4
ω
t
-
α
m
-
φ
2
R
I
S
C
,
(6d)
q
α
m
,
t
=
1
8
μ
0
F
C
2
+
F
d
2
2
2
Λ
0
2
+
Λ
s
2
+
4
F
C
2
+
F
d
2
2
Λ
0
Λ
s
cos
⁡
α
m
+
F
C
2
+
F
d
2
2
Λ
s
2
cos
⁡
2
α
m
+
F
C
F
d
2
-
4
Λ
0
Λ
s
cos
⁡
ω
t
+
β
1
-
2
φ
2
-
2
2
Λ
0
2
+
Λ
s
2
cos
⁡
ω
t
-
α
m
+
β
1
-
2
φ
2
-
Λ
s
2
cos
⁡
ω
t
+
α
m
+
β
1
-
2
φ
2
-
4
Λ
0
Λ
s
cos
⁡
ω
t
-
2
α
m
+
β
1
-
2
φ
2
-
Λ
s
2
cos
⁡
ω
t
-
3
α
m
+
β
1
-
2
φ
2
+
F
C
2
0.5
Λ
s
2
cos
⁡
2
ω
t
-
2
β
1
+
2
Λ
0
Λ
s
cos
⁡
2
ω
t
-
α
m
-
2
β
1
+
2
Λ
0
2
+
Λ
s
2
cos
⁡
2
ω
t
-
2
α
m
-
2
β
1
+
2
Λ
0
Λ
s
cos
⁡
2
ω
t
-
3
α
m
-
2
β
1
+
0.5
Λ
s
2
cos
⁡
2
ω
t
-
4
α
m
-
2
β
1
+
F
C
F
d
2
-
Λ
s
2
cos
⁡
3
ω
t
-
α
m
-
β
1
-
2
φ
2
-
4
Λ
0
Λ
s
cos
⁡
3
ω
t
-
2
α
m
-
β
1
-
2
φ
2
-
2
2
Λ
0
2
+
Λ
s
2
cos
⁡
3
ω
t
-
3
α
m
-
β
1
-
2
φ
2
-
4
Λ
0
Λ
s
cos
⁡
3
ω
t
-
4
α
m
-
β
1
-
2
φ
2
-
Λ
s
2
cos
⁡
3
ω
t
-
5
α
m
-
β
1
-
2
φ
2
+
F
d
2
2
0.5
Λ
s
2
cos
⁡
4
ω
t
-
2
α
m
-
4
φ
2
+
2
Λ
0
Λ
s
cos
⁡
4
ω
t
-
3
α
m
-
4
φ
2
+
2
Λ
0
2
+
Λ
s
2
cos
⁡
4
ω
t
-
4
α
m
-
4
φ
2
+
2
Λ
0
Λ
s
cos
⁡
4
ω
t
-
5
α
m
-
4
φ
2
+
0.5
Λ
s
2
cos
⁡
4
ω
t
-
6
α
m
-
4
φ
2
C
F
.As indicated in (6a)–(6d), MPPUA has different pulsating components under different performing conditions. Since the stator vibration is actually the response of the exciting MPPUA, the vibration spectrum should have the same harmonic components as MPPUA. Obviously, under normal condition and SAGE, the stator vibration has only 2nd harmonic components (the DC component force will not bring in vibrations to the stator but will induce a radial deformation tendency after a long action). The occurrence of SAGE will increase the vibration amplitude at 2f. However, when RISC or CF takes place, besides the 2nd harmonic components, 1st, 3rd, and 4th harmonic components will also be produced. To further study the exciting characteristics of MPPUA and the stator vibration response features, the upper amplitude expressions of each MPPUA component under different conditions are shown in Table 1, where I
f is the exciting current of the generator, f
s
d is the shorted degree of RISC, and δ
s is the relative SAGE value.Table 1
Upper amplitude expressions of MPPUA for different conditions.
Component
Performing condition
Amplitude formulas
Influential factors
DC component
Normal condition
F
1
2
Λ
0
2
/
4
μ
0
I
f
SAGE
F
1
2
Λ
0
+
Λ
s
2
/
4
μ
0
I
f, δ
s
RISC
(
F
C
2
+
F
d
2
2
)
Λ
0
2
/
4
μ
0
I
f, f
s
d
CF
(
F
C
2
+
F
d
2
2
)
Λ
0
+
Λ
s
2
/
4
μ
0
I
f, δ
s, f
s
d
1st harmonic
Normal condition
—
—
SAGE
—
—
RISC
-
F
C
F
d
2
Λ
0
2
/
2
μ
0
I
f, f
s
d
CF
F
C
F
d
2
Λ
0
+
Λ
s
2
/
2
μ
0
I
f, δ
s, f
s
d
2nd harmonic
Normal condition
F
1
2
Λ
0
2
/
4
μ
0
I
f
SAGE
F
1
2
Λ
0
+
Λ
s
2
/
4
μ
0
I
f, δ
s
RISC
F
C
2
Λ
0
2
/
4
μ
0
I
f, f
s
d
CF
F
C
2
Λ
0
+
Λ
s
2
/
4
μ
0
I
f, δ
s, f
s
d
3rd harmonic
Normal condition
—
—
SAGE
—
—
RISC
-
F
C
F
d
2
Λ
0
2
/
2
μ
0
I
f, f
s
d
CF
F
C
F
d
2
Λ
0
+
Λ
s
2
/
2
μ
0
I
f, δ
s, f
s
d
4th harmonic
Normal condition
—
—
SAGE
—
—
RISC
F
d
2
2
Λ
0
2
/
4
μ
0
I
f, f
s
d
CF
F
d
2
2
Λ
0
+
Λ
s
2
/
4
μ
0
I
f, δ
s, f
s
dAs shown in Table1, SAGE has larger MPPUA magnitude at 2f, while RISC has smaller MPPUA magnitude at 2f than normal condition. Specifically, CF has larger MPPUA amplitudes atf, 2f, 3f, and 4f than RISC. Consequently, the occurrence of SAGE will increase the 2nd harmonic vibration of stator, while RISC will decrease the 2nd harmonic vibration amplitude. The stator vibration amplitudes atf, 2f, 3f, and 4f under CF condition will be more intense than under RISC condition. This can be used for the fault identification among the single and the composite faults composed of SAGE and RISC.


## 3. Numerical Simulation and Experiment Study

### 3.1. Object and Method

The numerical FEM simulation and the experiment study are taken for a SDF-9 type nonsalient pole fault simulating generator (see Figure3(a)) in the State Key Lab of New Energy and Electric Power System, China, whose primary parameters are indicated in Table 2.Table 2
Primary parameters of SDF-9 type generator.
Parameter
Value
Rated capacity
7.5 kVA
Rated voltage
400 V
Power factor
0.8
Rated speed
n
r
=
3000 rpm
Number of pole pairs
p
=
1
Radial air-gap length
g
0
=
0.8 mm
Stator series conductors per phase
N
s
=
100
Axial length
L
0
=
100 mm
Number of stator slots
Z
1
=
24
Ratio of pitch to polar distance
K
y
=
y
/
τ
=
0.83
Pitch-shortening value
k
p
=
0.966
Distribution coefficient
k
d
=
0.958
Number of parallel branches
α
=
2
Number of exciting turns for each pole
N
f
=
480Figure 3
Study object of SDF-9 type generator.
(a)
Physical model of SDF-9 type generator
(b)
Method to set SAGE
(c)
Method to set RISC
(d)
Experimental testing system
(e)
2D finite element model
(f)
Coupling circuit of rotor winding for normal and SAGE cases
(g)
Coupling circuit of rotor winding for RISC and CF
(h)
Coupling circuit for stator windingsThe rotor of the generator is fixed by the bearing block, while the stator can be moved along the horizontally radial direction by adjusting the four screws on the generator to simulate SAGE faults. The movement performance can be controlled by the two dial indicators, as shown in Figure3(b). Outside the generator, there is a plate with shorted taps of the exciting windings, as indicated in Figure 3(c). RISC can be simulated by connecting different taps. Also, CF conditions with different faulty degrees can be applied via setting different SAGE values and connecting different taps at the same time. During the experiment, the exciting current is set to 0.8 A, the rotating speed of the rotor is set to 3000 rpm (the rotary period is 20 ms and the frequency is 50 Hz), and the line voltage is 380 V. The experimental testing system is indicated in Figure 3(d).Objectively, there are some differences to set the velocity sensors in different positions. The general rigidities in the horizontal direction and the vertical direction are different (the vertical direction has a larger rigidity because the foundation is in this direction and therefore sensors here will sample smaller vibration amplitudes). What is more, since the stator is moved along the horizontal direction, the magnetic flux density is larger on one side in this direction but smaller on the other side. So, the MPPUA density is actually larger on the side which has the minimum air-gap length but smaller on the opposite side. Consequently, the sensors set on different positions will have varied vibration amplitudes. However, no matter where the sensors are set, the developing tendency of the stator vibration will be the same due to the uniform exciting force indicated in (6a)–(6d).The finite element model is built up, setting the performing parameters the same as the experiment, as indicated in Figure3(e). The corresponding external coupling circuits for the exciting windings and the stator windings are illustrated in Figures 3(f), 3(g), and 3(h).The experiment work and the FEM simulation study are gradually taken by following the four steps.(1) Normal Performance. The generator performs in normal condition without setting SAGE or RISC, and the stator vibration data is collected as a comparing reference. In addition, the MPPUA in normal condition on the stator is also calculated through the FEM simulation.(2) SAGE Cases. 0.1 mm (12.5%), 0.2 mm (25%), and 0.3 mm (37.5%) SAGEs are set each time, respectively, both in the experiment performance and in the FEM simulation. For the simulation, the rotor and the exciting windings are shifted along the x-axis to simulate different SAGE conditions (see Figure 3(e)). Experimental stator vibration signals and calculated MPPUA data are collected for further study.(3) RISC Cases. 3%, 6%, and 12% RISC are, respectively, set in the experiments by connecting L
1
L
2, L
4
L
5, and L
2
L
3. Also, the same RISC degrees are set in the FEM simulation by adjusting the values of L
Field5-shorted and L
Field5-left indicated in Figure 3(g). Correspondingly, the conductors in the shorted slot of the FEM model are divided into two parts. One is the shorted part, and the other is the left part, as indicated in Figure 3(e).(4) CF Cases. Firstly, 0.1 mm SAGE is set up, and 3%, 6%, and 12% RISC are set each time, respectively, both in the experiments and in the simulations. Secondly, 3% RISC is set up, and 0.1 mm, 0.3 mm, and 0.5 mm SAGE conditions are applied each time, respectively. By doing this, the impacts of SAGE and the effects of RISC on MPPUA and the stator vibrations under CF conditions can be obtained.


### 3.2. Results and Discussion

#### 3.2.1. Pass-Band Results

MPPUA distributions on stator under different performing conditions obtained by FEM calculation are indicated in Figure4. It is shown that the district near the pole has a much more intense MPPUA, while at other positions MPPUA has a very little value. This is because the magnetic lines near the poles have the strongest intensity. In normal condition, the MPPUA distribution is of symmetry, while the occurrence of SAGE, RISC, or CF will break this symmetry. As SAGE increases, MPPUA will be increased, as indicated in Figures 4(a)–4(d). It is also indicated that the very place which has the largest MPPUA is generally in accordance with the position where the radial air-gap length is the minimum. This is caused due to the max permeance in this position; see (1) and Figure 1(b).Figure 4
MPPUA distribution under different conditions.
(a)
Normal condition
(b)
0.1 mm SAGE
(c)
0.2 mm SAGE
(d)
0.3 mm SAGE
(e)
3% RISC
(f)
6% RISC
(g)
12% RISC
(h)
0.1 mm SAGE and 3% RISC
(i)
0.1 mm SAGE and 6% RISC
(j)
0.1 mm SAGE and 12% RISC
(k)
0.2 mm SAGE and 3% RISC
(l)
0.3 mm SAGE and 3% RISCHowever, when RISC takes place, MPPUA will be decreased, as indicated in Figures4(a) and 4(e). This is because RISC decreases the effective exciting ampere turns. This can be also explained by comparing Figure 1(c) with Figure 1(d). The primary MMF F
C under RISC (see Figure 1(d)) is actually smaller than F
1 in normal condition (see Figure 1(c)) due to the effect of the induced inverse MMF F
d
1. The more serious RISC is, the more MPPUA will be decreased, as indicated in Figures 4(e)–4(g).Comparing Figure4(h) with Figures 4(b) and 4(e), it is obvious that MPPUA under CF is smaller than that under SAGE but meanwhile larger than that under RISC. Besides, as SAGE increases, MPPUA under CF will also be increased, as indicated in Figures 4(h), 4(k), and 4(l). However, the development of RISC will decrease MPPUA in general, as illustrated in Figures 1(h)–1(j). This means RISC will generally decrease MFD while SAGE will generally increase MFD, which follows the previous theoretical analysis in Section 2.1.To show the developing tendency of MPPUA more clearly, the time domain curves for a stable period obtained from FEM calculations for each performing condition are indicated in Figure5. It is shown that, under the single SAGE fault, the increment of SAGE will raise the value of MPPUA, as shown in Figure 5(a). On the contrary, the occurrence and the development of RISC will generally bring down the value of MPPUA (the mean value and the RMS value are both decreased), as indicated in Figure 5(b).Figure 5
Time domain curves of MPPUA under different conditions.
(a)
MPPUA under different SAGE conditions
(b)
MPPUA under different RISC conditions
(c)
MPPUA under CFs with different SAGE values
(d)
MPPUA under CFs with different RISC degreesFor the CF cases, the increment of SAGE will increase MPPUA (see Figure5(c)), while the development of RISC will decrease MPPUA (see Figure 5(d)). This developing trend is in accordance with the single faults. Comparatively, MPPUA under CF is larger than that under the single RISC fault, as indicated in Figure 5(c). However, MPPUA under CF is smaller than that under the single SAGE fault, as illustrated in Figure 5(d). This also means that SAGE will generally increase MFD while RISC will primarily decrease MFD, which again confirms the theoretical analysis in Section 2.1.Correspondingly, the stator vibration intensity, which is computed via (7), is shown in Figure 6. In (7), y
i is the vibration speed, m is the total number of sampling points, and y is the vibration intensity. Hence,(7)
y
=
∑
i
=
1
m
y
i
2
m
.Figure 6
Vibration intensity under different performing conditions.
(a)
Vibration intensity under different SAGE conditions
(b)
Vibration intensity under different RISC conditionsAs indicated in Figure6, it is clear that whether under the single SAGE fault or CF, the increment of SAGE will increase the stator vibration intensity. However, the development of RISC will decrease the stator vibration intensity. In addition, it is also suggested from Figure 6 that the vibration intensity under CF is smaller than that under the single SAGE fault but meanwhile larger than that under the single RISC fault. This is in accordance with the qualitative result obtained in the theoretical analysis and the MPPUA data presented above.


#### 3.2.2. Special-Frequency Component Results

To further study the impact of different faulty kinds on the stator vibration characteristics, special-frequency components of MPPUA and vibration, including the 1st, 2nd, 3rd, and 4th harmonic components, are investigated as well. The MPPUA amplitudes for each harmonic component under different performing conditions are indicated in Figure7, while the stator vibration spectra are shown in Figure 8.Figure 7
Spectra of MPPUA under different conditions.
(a)
Normal condition
(b)
0.1 mm SAGE
(c)
0.2 mm SAGE
(d)
0.3 mm SAGE
(e)
3% RISC
(f)
6% RISC
(g)
12% RISC
(h)
0.1 mm SAGE and 3% RISC
(i)
0.1 mm SAGE and 6% RISC
(j)
0.1 mm SAGE and 12% RISC
(k)
3% RISC and 0.2 mm SAGE
(l)
3% RISC and 0.3 mm SAGEFigure 8
Tested stator vibration spectra under different conditions.
(a)
Normal condition
(b)
0.1 mm SAGE
(c)
0.2 mm SAGE
(d)
0.3 mm SAGE
(e)
3% RISC
(f)
6% RISC
(g)
12% RISC
(h)
0.1 mm SAGE and 3% RISC
(i)
0.1 mm SAGE and 6% RISC
(j)
0.1 mm SAGE and 12% RISC
(k)
0.2 mm SAGE and 3% RISC
(l)
0.3 mm SAGE and 3% RISCIt is suggested from Figure7(a) that, in normal condition, MPPUA mainly has a DC component and a 2nd harmonic component, which well follows the theoretical result indicated in (6a)–(6d). Actually, there is still a tiny 4th harmonic component. The very reason for this extra 4th harmonic component is because MPPUA is the square result of MFD (see (5)) which has not only the fundamental-frequency component but also the other odd harmonics. Consequently, MPPUA should theoretically have each even harmonic component due to the square operation, with the even harmonic components’ amplitudes decreased as the harmonic order increases. Equations (6a)–(6d) only consider the 1st harmonic but ignore the higher harmonics due to their tiny values. For the sake of convenience, in this paper, the higher order harmonics are not taken into account. Comparing Figure 7(a) with Figures 7(b)–7(d), it is shown that as SAGE happens and increases, both the DC component and the 2nd harmonic component of MPPUA will be increased. This is consistent with the previous analysis.As illustrated in Figures7(a) and 7(e)–7(g), the occurrence and development of RISC will generally increase the 1st, 3rd, and 4th harmonic components but meanwhile decrease the 2nd harmonic component. This can be qualitatively explained by Table 1. As indicated in Table 1, normally, there are no 1st, 3rd, and 4th harmonic components, while under RISC the 1st, 2nd, 3rd, and 4th harmonic components appear. Therefore, the new components brought in by RISC will be increased. Moreover, the MPPUA amplitude in normal condition is F
1
2
Λ
0
2
/
4
μ
0, while under RISC the amplitude is F
C
2
Λ
0
2
/
4
μ
0. As illustrated in Figures 1(c) and 1(d), it is obvious that F
C is smaller than F
1, resulting in the decrease of the 2nd harmonic component of MPPUA.Comparing Figure7(h) with Figure 7(b), Figure 7(k) with Figure 7(c), and Figure 7(l) with Figure 7(d), it can be found that MPPUA under CF has a smaller value at 2f (f is the electrical frequency) but meanwhile has a larger value atf, 3f, and 4f than under the single SAGE fault. This again confirms the conclusion presented in the previous paragraph that RISC will increase the 1st, 3rd, and 4th harmonic components but meanwhile decrease the 2nd harmonic component. In addition, comparing Figure 7(h) with Figure 7(e), Figure 7(i) with Figure 7(f), and Figure 7(j) with Figure 7(g), it is shown that the 1st to the 4th harmonic components of MPPUA under CF are all larger than those under RISC. This means SAGE will generally increase MFD, which has been found out previously. Actually, the amplitude formulas indicated in Table 1 can also explain this well, for the permeance under CF is (Λ
0
+
Λ
s), while the permeance under RISC is only Λ
0 (see Table 1).Taking MPPUA as the exciting force, the stator vibration can be treated as the response. As indicated in Figure8, the stator vibration tendency at each harmonic frequency well follows the developing trend of MPPUA. Specifically, Figure 8(a) shows that the stator vibration in normal condition not only has each even harmonic component (primarily the 2nd and the 4th harmonics) but also includes each odd harmonic component (primarily the 1st, 3rd, and 5th harmonics). In theory, as analyzed previously, there should be only even harmonic components existing (primarily the 2nd harmonic). The extra odd harmonic components of the stator vibration are mainly transferred from the rotor vibration (the rotor and the stator both located on the basis; see Figure 3(a)) and caused by the initial asymmetry inside the generator. To study the essential effect of each kind of fault on the stator vibration, the vibration amplitudes of each harmonic in normal condition are treated as the null drifts of the experiment system, and the faulty vibration amplitudes are subtracted by these null drifts. For example, comparing with the normal condition, vibration amplitude at 2f for 0.1 mm, 0.2 mm, and 0.3 mm SAGE increases by 32.9% (0.886 mm/s), 50.5% (1.359 mm/s), and 70.9% (1.909 mm/s), respectively. This indicates that these increments of the vibration amplitude are the essential impact caused by the three SAGE fault conditions.To better show the relation between the input excitation force and the output vibration response, the line charts of MPPUA and the stator vibration at each frequency under different running conditions are illustrated in Figure9. It is shown that the developing tendency of the tested stator vibration amplitudes at each harmonic frequency generally accords with the changing trend of MPPUA. Meanwhile, it is also clear that as SAGE increases, both MPPUA and the vibration under CF have a larger value atf, 3f, and 4f but in the meantime have a smaller value at 2f than those under the single SAGE fault. However, as RISC develops, both MPPUA and the stator vibration will have a larger value under the CF condition than under the single RISC fault. These results are in good accordance with the conclusions obtained previously, confirming that both the FEM calculation and the experiment data match the previous analysis. In addition, this also indicates that the stator vibration response is consistent with the exciting MPPUA.Figure 9
Comparison between MPPUA and tested stator vibration for different conditions.
(a)
MPPUA when SAGE varies
(b)
Vibration when SAGE varies
(c)
MPPUA when RISC develops
(d)
Vibration when RISC develops


#### 3.2.3. Fault Identification Criterion

Based on the theoretical analysis, the numerical FEM calculation, and the experiment study, it is found that the stator vibration characteristic varies under different faulty conditions. This can be employed to develop an identification criterion for the single and the composite faults composed of SAGE and RISC. More details can be found in Table3.Table 3
Fault identification criterion based on stator vibration characteristics.
Stator vibration characteristics
Performing condition
Having only soft 2nd harmonic vibrations
Normal condition
The vibration at 2f is increased, while the other components generally keep stable
SAGE exists
The vibration at 2f is decreased, but meanwhile vibrations at f, 3f, and 4fare increased
RISC exists
The vibration at 2f is firstly decreased and then increased; meanwhile, vibrations at f, 3f, and 4fare increased
CF exists


## 3.1. Object and Method

The numerical FEM simulation and the experiment study are taken for a SDF-9 type nonsalient pole fault simulating generator (see Figure3(a)) in the State Key Lab of New Energy and Electric Power System, China, whose primary parameters are indicated in Table 2.Table 2
Primary parameters of SDF-9 type generator.
Parameter
Value
Rated capacity
7.5 kVA
Rated voltage
400 V
Power factor
0.8
Rated speed
n
r
=
3000 rpm
Number of pole pairs
p
=
1
Radial air-gap length
g
0
=
0.8 mm
Stator series conductors per phase
N
s
=
100
Axial length
L
0
=
100 mm
Number of stator slots
Z
1
=
24
Ratio of pitch to polar distance
K
y
=
y
/
τ
=
0.83
Pitch-shortening value
k
p
=
0.966
Distribution coefficient
k
d
=
0.958
Number of parallel branches
α
=
2
Number of exciting turns for each pole
N
f
=
480Figure 3
Study object of SDF-9 type generator.
(a)
Physical model of SDF-9 type generator
(b)
Method to set SAGE
(c)
Method to set RISC
(d)
Experimental testing system
(e)
2D finite element model
(f)
Coupling circuit of rotor winding for normal and SAGE cases
(g)
Coupling circuit of rotor winding for RISC and CF
(h)
Coupling circuit for stator windingsThe rotor of the generator is fixed by the bearing block, while the stator can be moved along the horizontally radial direction by adjusting the four screws on the generator to simulate SAGE faults. The movement performance can be controlled by the two dial indicators, as shown in Figure3(b). Outside the generator, there is a plate with shorted taps of the exciting windings, as indicated in Figure 3(c). RISC can be simulated by connecting different taps. Also, CF conditions with different faulty degrees can be applied via setting different SAGE values and connecting different taps at the same time. During the experiment, the exciting current is set to 0.8 A, the rotating speed of the rotor is set to 3000 rpm (the rotary period is 20 ms and the frequency is 50 Hz), and the line voltage is 380 V. The experimental testing system is indicated in Figure 3(d).Objectively, there are some differences to set the velocity sensors in different positions. The general rigidities in the horizontal direction and the vertical direction are different (the vertical direction has a larger rigidity because the foundation is in this direction and therefore sensors here will sample smaller vibration amplitudes). What is more, since the stator is moved along the horizontal direction, the magnetic flux density is larger on one side in this direction but smaller on the other side. So, the MPPUA density is actually larger on the side which has the minimum air-gap length but smaller on the opposite side. Consequently, the sensors set on different positions will have varied vibration amplitudes. However, no matter where the sensors are set, the developing tendency of the stator vibration will be the same due to the uniform exciting force indicated in (6a)–(6d).The finite element model is built up, setting the performing parameters the same as the experiment, as indicated in Figure3(e). The corresponding external coupling circuits for the exciting windings and the stator windings are illustrated in Figures 3(f), 3(g), and 3(h).The experiment work and the FEM simulation study are gradually taken by following the four steps.(1) Normal Performance. The generator performs in normal condition without setting SAGE or RISC, and the stator vibration data is collected as a comparing reference. In addition, the MPPUA in normal condition on the stator is also calculated through the FEM simulation.(2) SAGE Cases. 0.1 mm (12.5%), 0.2 mm (25%), and 0.3 mm (37.5%) SAGEs are set each time, respectively, both in the experiment performance and in the FEM simulation. For the simulation, the rotor and the exciting windings are shifted along the x-axis to simulate different SAGE conditions (see Figure 3(e)). Experimental stator vibration signals and calculated MPPUA data are collected for further study.(3) RISC Cases. 3%, 6%, and 12% RISC are, respectively, set in the experiments by connecting L
1
L
2, L
4
L
5, and L
2
L
3. Also, the same RISC degrees are set in the FEM simulation by adjusting the values of L
Field5-shorted and L
Field5-left indicated in Figure 3(g). Correspondingly, the conductors in the shorted slot of the FEM model are divided into two parts. One is the shorted part, and the other is the left part, as indicated in Figure 3(e).(4) CF Cases. Firstly, 0.1 mm SAGE is set up, and 3%, 6%, and 12% RISC are set each time, respectively, both in the experiments and in the simulations. Secondly, 3% RISC is set up, and 0.1 mm, 0.3 mm, and 0.5 mm SAGE conditions are applied each time, respectively. By doing this, the impacts of SAGE and the effects of RISC on MPPUA and the stator vibrations under CF conditions can be obtained.


## 3.2. Results and Discussion

### 3.2.1. Pass-Band Results

MPPUA distributions on stator under different performing conditions obtained by FEM calculation are indicated in Figure4. It is shown that the district near the pole has a much more intense MPPUA, while at other positions MPPUA has a very little value. This is because the magnetic lines near the poles have the strongest intensity. In normal condition, the MPPUA distribution is of symmetry, while the occurrence of SAGE, RISC, or CF will break this symmetry. As SAGE increases, MPPUA will be increased, as indicated in Figures 4(a)–4(d). It is also indicated that the very place which has the largest MPPUA is generally in accordance with the position where the radial air-gap length is the minimum. This is caused due to the max permeance in this position; see (1) and Figure 1(b).Figure 4
MPPUA distribution under different conditions.
(a)
Normal condition
(b)
0.1 mm SAGE
(c)
0.2 mm SAGE
(d)
0.3 mm SAGE
(e)
3% RISC
(f)
6% RISC
(g)
12% RISC
(h)
0.1 mm SAGE and 3% RISC
(i)
0.1 mm SAGE and 6% RISC
(j)
0.1 mm SAGE and 12% RISC
(k)
0.2 mm SAGE and 3% RISC
(l)
0.3 mm SAGE and 3% RISCHowever, when RISC takes place, MPPUA will be decreased, as indicated in Figures4(a) and 4(e). This is because RISC decreases the effective exciting ampere turns. This can be also explained by comparing Figure 1(c) with Figure 1(d). The primary MMF F
C under RISC (see Figure 1(d)) is actually smaller than F
1 in normal condition (see Figure 1(c)) due to the effect of the induced inverse MMF F
d
1. The more serious RISC is, the more MPPUA will be decreased, as indicated in Figures 4(e)–4(g).Comparing Figure4(h) with Figures 4(b) and 4(e), it is obvious that MPPUA under CF is smaller than that under SAGE but meanwhile larger than that under RISC. Besides, as SAGE increases, MPPUA under CF will also be increased, as indicated in Figures 4(h), 4(k), and 4(l). However, the development of RISC will decrease MPPUA in general, as illustrated in Figures 1(h)–1(j). This means RISC will generally decrease MFD while SAGE will generally increase MFD, which follows the previous theoretical analysis in Section 2.1.To show the developing tendency of MPPUA more clearly, the time domain curves for a stable period obtained from FEM calculations for each performing condition are indicated in Figure5. It is shown that, under the single SAGE fault, the increment of SAGE will raise the value of MPPUA, as shown in Figure 5(a). On the contrary, the occurrence and the development of RISC will generally bring down the value of MPPUA (the mean value and the RMS value are both decreased), as indicated in Figure 5(b).Figure 5
Time domain curves of MPPUA under different conditions.
(a)
MPPUA under different SAGE conditions
(b)
MPPUA under different RISC conditions
(c)
MPPUA under CFs with different SAGE values
(d)
MPPUA under CFs with different RISC degreesFor the CF cases, the increment of SAGE will increase MPPUA (see Figure5(c)), while the development of RISC will decrease MPPUA (see Figure 5(d)). This developing trend is in accordance with the single faults. Comparatively, MPPUA under CF is larger than that under the single RISC fault, as indicated in Figure 5(c). However, MPPUA under CF is smaller than that under the single SAGE fault, as illustrated in Figure 5(d). This also means that SAGE will generally increase MFD while RISC will primarily decrease MFD, which again confirms the theoretical analysis in Section 2.1.Correspondingly, the stator vibration intensity, which is computed via (7), is shown in Figure 6. In (7), y
i is the vibration speed, m is the total number of sampling points, and y is the vibration intensity. Hence,(7)
y
=
∑
i
=
1
m
y
i
2
m
.Figure 6
Vibration intensity under different performing conditions.
(a)
Vibration intensity under different SAGE conditions
(b)
Vibration intensity under different RISC conditionsAs indicated in Figure6, it is clear that whether under the single SAGE fault or CF, the increment of SAGE will increase the stator vibration intensity. However, the development of RISC will decrease the stator vibration intensity. In addition, it is also suggested from Figure 6 that the vibration intensity under CF is smaller than that under the single SAGE fault but meanwhile larger than that under the single RISC fault. This is in accordance with the qualitative result obtained in the theoretical analysis and the MPPUA data presented above.


### 3.2.2. Special-Frequency Component Results

To further study the impact of different faulty kinds on the stator vibration characteristics, special-frequency components of MPPUA and vibration, including the 1st, 2nd, 3rd, and 4th harmonic components, are investigated as well. The MPPUA amplitudes for each harmonic component under different performing conditions are indicated in Figure7, while the stator vibration spectra are shown in Figure 8.Figure 7
Spectra of MPPUA under different conditions.
(a)
Normal condition
(b)
0.1 mm SAGE
(c)
0.2 mm SAGE
(d)
0.3 mm SAGE
(e)
3% RISC
(f)
6% RISC
(g)
12% RISC
(h)
0.1 mm SAGE and 3% RISC
(i)
0.1 mm SAGE and 6% RISC
(j)
0.1 mm SAGE and 12% RISC
(k)
3% RISC and 0.2 mm SAGE
(l)
3% RISC and 0.3 mm SAGEFigure 8
Tested stator vibration spectra under different conditions.
(a)
Normal condition
(b)
0.1 mm SAGE
(c)
0.2 mm SAGE
(d)
0.3 mm SAGE
(e)
3% RISC
(f)
6% RISC
(g)
12% RISC
(h)
0.1 mm SAGE and 3% RISC
(i)
0.1 mm SAGE and 6% RISC
(j)
0.1 mm SAGE and 12% RISC
(k)
0.2 mm SAGE and 3% RISC
(l)
0.3 mm SAGE and 3% RISCIt is suggested from Figure7(a) that, in normal condition, MPPUA mainly has a DC component and a 2nd harmonic component, which well follows the theoretical result indicated in (6a)–(6d). Actually, there is still a tiny 4th harmonic component. The very reason for this extra 4th harmonic component is because MPPUA is the square result of MFD (see (5)) which has not only the fundamental-frequency component but also the other odd harmonics. Consequently, MPPUA should theoretically have each even harmonic component due to the square operation, with the even harmonic components’ amplitudes decreased as the harmonic order increases. Equations (6a)–(6d) only consider the 1st harmonic but ignore the higher harmonics due to their tiny values. For the sake of convenience, in this paper, the higher order harmonics are not taken into account. Comparing Figure 7(a) with Figures 7(b)–7(d), it is shown that as SAGE happens and increases, both the DC component and the 2nd harmonic component of MPPUA will be increased. This is consistent with the previous analysis.As illustrated in Figures7(a) and 7(e)–7(g), the occurrence and development of RISC will generally increase the 1st, 3rd, and 4th harmonic components but meanwhile decrease the 2nd harmonic component. This can be qualitatively explained by Table 1. As indicated in Table 1, normally, there are no 1st, 3rd, and 4th harmonic components, while under RISC the 1st, 2nd, 3rd, and 4th harmonic components appear. Therefore, the new components brought in by RISC will be increased. Moreover, the MPPUA amplitude in normal condition is F
1
2
Λ
0
2
/
4
μ
0, while under RISC the amplitude is F
C
2
Λ
0
2
/
4
μ
0. As illustrated in Figures 1(c) and 1(d), it is obvious that F
C is smaller than F
1, resulting in the decrease of the 2nd harmonic component of MPPUA.Comparing Figure7(h) with Figure 7(b), Figure 7(k) with Figure 7(c), and Figure 7(l) with Figure 7(d), it can be found that MPPUA under CF has a smaller value at 2f (f is the electrical frequency) but meanwhile has a larger value atf, 3f, and 4f than under the single SAGE fault. This again confirms the conclusion presented in the previous paragraph that RISC will increase the 1st, 3rd, and 4th harmonic components but meanwhile decrease the 2nd harmonic component. In addition, comparing Figure 7(h) with Figure 7(e), Figure 7(i) with Figure 7(f), and Figure 7(j) with Figure 7(g), it is shown that the 1st to the 4th harmonic components of MPPUA under CF are all larger than those under RISC. This means SAGE will generally increase MFD, which has been found out previously. Actually, the amplitude formulas indicated in Table 1 can also explain this well, for the permeance under CF is (Λ
0
+
Λ
s), while the permeance under RISC is only Λ
0 (see Table 1).Taking MPPUA as the exciting force, the stator vibration can be treated as the response. As indicated in Figure8, the stator vibration tendency at each harmonic frequency well follows the developing trend of MPPUA. Specifically, Figure 8(a) shows that the stator vibration in normal condition not only has each even harmonic component (primarily the 2nd and the 4th harmonics) but also includes each odd harmonic component (primarily the 1st, 3rd, and 5th harmonics). In theory, as analyzed previously, there should be only even harmonic components existing (primarily the 2nd harmonic). The extra odd harmonic components of the stator vibration are mainly transferred from the rotor vibration (the rotor and the stator both located on the basis; see Figure 3(a)) and caused by the initial asymmetry inside the generator. To study the essential effect of each kind of fault on the stator vibration, the vibration amplitudes of each harmonic in normal condition are treated as the null drifts of the experiment system, and the faulty vibration amplitudes are subtracted by these null drifts. For example, comparing with the normal condition, vibration amplitude at 2f for 0.1 mm, 0.2 mm, and 0.3 mm SAGE increases by 32.9% (0.886 mm/s), 50.5% (1.359 mm/s), and 70.9% (1.909 mm/s), respectively. This indicates that these increments of the vibration amplitude are the essential impact caused by the three SAGE fault conditions.To better show the relation between the input excitation force and the output vibration response, the line charts of MPPUA and the stator vibration at each frequency under different running conditions are illustrated in Figure9. It is shown that the developing tendency of the tested stator vibration amplitudes at each harmonic frequency generally accords with the changing trend of MPPUA. Meanwhile, it is also clear that as SAGE increases, both MPPUA and the vibration under CF have a larger value atf, 3f, and 4f but in the meantime have a smaller value at 2f than those under the single SAGE fault. However, as RISC develops, both MPPUA and the stator vibration will have a larger value under the CF condition than under the single RISC fault. These results are in good accordance with the conclusions obtained previously, confirming that both the FEM calculation and the experiment data match the previous analysis. In addition, this also indicates that the stator vibration response is consistent with the exciting MPPUA.Figure 9
Comparison between MPPUA and tested stator vibration for different conditions.
(a)
MPPUA when SAGE varies
(b)
Vibration when SAGE varies
(c)
MPPUA when RISC develops
(d)
Vibration when RISC develops


### 3.2.3. Fault Identification Criterion

Based on the theoretical analysis, the numerical FEM calculation, and the experiment study, it is found that the stator vibration characteristic varies under different faulty conditions. This can be employed to develop an identification criterion for the single and the composite faults composed of SAGE and RISC. More details can be found in Table3.Table 3
Fault identification criterion based on stator vibration characteristics.
Stator vibration characteristics
Performing condition
Having only soft 2nd harmonic vibrations
Normal condition
The vibration at 2f is increased, while the other components generally keep stable
SAGE exists
The vibration at 2f is decreased, but meanwhile vibrations at f, 3f, and 4fare increased
RISC exists
The vibration at 2f is firstly decreased and then increased; meanwhile, vibrations at f, 3f, and 4fare increased
CF exists


## 3.2.1. Pass-Band Results

MPPUA distributions on stator under different performing conditions obtained by FEM calculation are indicated in Figure4. It is shown that the district near the pole has a much more intense MPPUA, while at other positions MPPUA has a very little value. This is because the magnetic lines near the poles have the strongest intensity. In normal condition, the MPPUA distribution is of symmetry, while the occurrence of SAGE, RISC, or CF will break this symmetry. As SAGE increases, MPPUA will be increased, as indicated in Figures 4(a)–4(d). It is also indicated that the very place which has the largest MPPUA is generally in accordance with the position where the radial air-gap length is the minimum. This is caused due to the max permeance in this position; see (1) and Figure 1(b).Figure 4
MPPUA distribution under different conditions.
(a)
Normal condition
(b)
0.1 mm SAGE
(c)
0.2 mm SAGE
(d)
0.3 mm SAGE
(e)
3% RISC
(f)
6% RISC
(g)
12% RISC
(h)
0.1 mm SAGE and 3% RISC
(i)
0.1 mm SAGE and 6% RISC
(j)
0.1 mm SAGE and 12% RISC
(k)
0.2 mm SAGE and 3% RISC
(l)
0.3 mm SAGE and 3% RISCHowever, when RISC takes place, MPPUA will be decreased, as indicated in Figures4(a) and 4(e). This is because RISC decreases the effective exciting ampere turns. This can be also explained by comparing Figure 1(c) with Figure 1(d). The primary MMF F
C under RISC (see Figure 1(d)) is actually smaller than F
1 in normal condition (see Figure 1(c)) due to the effect of the induced inverse MMF F
d
1. The more serious RISC is, the more MPPUA will be decreased, as indicated in Figures 4(e)–4(g).Comparing Figure4(h) with Figures 4(b) and 4(e), it is obvious that MPPUA under CF is smaller than that under SAGE but meanwhile larger than that under RISC. Besides, as SAGE increases, MPPUA under CF will also be increased, as indicated in Figures 4(h), 4(k), and 4(l). However, the development of RISC will decrease MPPUA in general, as illustrated in Figures 1(h)–1(j). This means RISC will generally decrease MFD while SAGE will generally increase MFD, which follows the previous theoretical analysis in Section 2.1.To show the developing tendency of MPPUA more clearly, the time domain curves for a stable period obtained from FEM calculations for each performing condition are indicated in Figure5. It is shown that, under the single SAGE fault, the increment of SAGE will raise the value of MPPUA, as shown in Figure 5(a). On the contrary, the occurrence and the development of RISC will generally bring down the value of MPPUA (the mean value and the RMS value are both decreased), as indicated in Figure 5(b).Figure 5
Time domain curves of MPPUA under different conditions.
(a)
MPPUA under different SAGE conditions
(b)
MPPUA under different RISC conditions
(c)
MPPUA under CFs with different SAGE values
(d)
MPPUA under CFs with different RISC degreesFor the CF cases, the increment of SAGE will increase MPPUA (see Figure5(c)), while the development of RISC will decrease MPPUA (see Figure 5(d)). This developing trend is in accordance with the single faults. Comparatively, MPPUA under CF is larger than that under the single RISC fault, as indicated in Figure 5(c). However, MPPUA under CF is smaller than that under the single SAGE fault, as illustrated in Figure 5(d). This also means that SAGE will generally increase MFD while RISC will primarily decrease MFD, which again confirms the theoretical analysis in Section 2.1.Correspondingly, the stator vibration intensity, which is computed via (7), is shown in Figure 6. In (7), y
i is the vibration speed, m is the total number of sampling points, and y is the vibration intensity. Hence,(7)
y
=
∑
i
=
1
m
y
i
2
m
.Figure 6
Vibration intensity under different performing conditions.
(a)
Vibration intensity under different SAGE conditions
(b)
Vibration intensity under different RISC conditionsAs indicated in Figure6, it is clear that whether under the single SAGE fault or CF, the increment of SAGE will increase the stator vibration intensity. However, the development of RISC will decrease the stator vibration intensity. In addition, it is also suggested from Figure 6 that the vibration intensity under CF is smaller than that under the single SAGE fault but meanwhile larger than that under the single RISC fault. This is in accordance with the qualitative result obtained in the theoretical analysis and the MPPUA data presented above.


## 3.2.2. Special-Frequency Component Results

To further study the impact of different faulty kinds on the stator vibration characteristics, special-frequency components of MPPUA and vibration, including the 1st, 2nd, 3rd, and 4th harmonic components, are investigated as well. The MPPUA amplitudes for each harmonic component under different performing conditions are indicated in Figure7, while the stator vibration spectra are shown in Figure 8.Figure 7
Spectra of MPPUA under different conditions.
(a)
Normal condition
(b)
0.1 mm SAGE
(c)
0.2 mm SAGE
(d)
0.3 mm SAGE
(e)
3% RISC
(f)
6% RISC
(g)
12% RISC
(h)
0.1 mm SAGE and 3% RISC
(i)
0.1 mm SAGE and 6% RISC
(j)
0.1 mm SAGE and 12% RISC
(k)
3% RISC and 0.2 mm SAGE
(l)
3% RISC and 0.3 mm SAGEFigure 8
Tested stator vibration spectra under different conditions.
(a)
Normal condition
(b)
0.1 mm SAGE
(c)
0.2 mm SAGE
(d)
0.3 mm SAGE
(e)
3% RISC
(f)
6% RISC
(g)
12% RISC
(h)
0.1 mm SAGE and 3% RISC
(i)
0.1 mm SAGE and 6% RISC
(j)
0.1 mm SAGE and 12% RISC
(k)
0.2 mm SAGE and 3% RISC
(l)
0.3 mm SAGE and 3% RISCIt is suggested from Figure7(a) that, in normal condition, MPPUA mainly has a DC component and a 2nd harmonic component, which well follows the theoretical result indicated in (6a)–(6d). Actually, there is still a tiny 4th harmonic component. The very reason for this extra 4th harmonic component is because MPPUA is the square result of MFD (see (5)) which has not only the fundamental-frequency component but also the other odd harmonics. Consequently, MPPUA should theoretically have each even harmonic component due to the square operation, with the even harmonic components’ amplitudes decreased as the harmonic order increases. Equations (6a)–(6d) only consider the 1st harmonic but ignore the higher harmonics due to their tiny values. For the sake of convenience, in this paper, the higher order harmonics are not taken into account. Comparing Figure 7(a) with Figures 7(b)–7(d), it is shown that as SAGE happens and increases, both the DC component and the 2nd harmonic component of MPPUA will be increased. This is consistent with the previous analysis.As illustrated in Figures7(a) and 7(e)–7(g), the occurrence and development of RISC will generally increase the 1st, 3rd, and 4th harmonic components but meanwhile decrease the 2nd harmonic component. This can be qualitatively explained by Table 1. As indicated in Table 1, normally, there are no 1st, 3rd, and 4th harmonic components, while under RISC the 1st, 2nd, 3rd, and 4th harmonic components appear. Therefore, the new components brought in by RISC will be increased. Moreover, the MPPUA amplitude in normal condition is F
1
2
Λ
0
2
/
4
μ
0, while under RISC the amplitude is F
C
2
Λ
0
2
/
4
μ
0. As illustrated in Figures 1(c) and 1(d), it is obvious that F
C is smaller than F
1, resulting in the decrease of the 2nd harmonic component of MPPUA.Comparing Figure7(h) with Figure 7(b), Figure 7(k) with Figure 7(c), and Figure 7(l) with Figure 7(d), it can be found that MPPUA under CF has a smaller value at 2f (f is the electrical frequency) but meanwhile has a larger value atf, 3f, and 4f than under the single SAGE fault. This again confirms the conclusion presented in the previous paragraph that RISC will increase the 1st, 3rd, and 4th harmonic components but meanwhile decrease the 2nd harmonic component. In addition, comparing Figure 7(h) with Figure 7(e), Figure 7(i) with Figure 7(f), and Figure 7(j) with Figure 7(g), it is shown that the 1st to the 4th harmonic components of MPPUA under CF are all larger than those under RISC. This means SAGE will generally increase MFD, which has been found out previously. Actually, the amplitude formulas indicated in Table 1 can also explain this well, for the permeance under CF is (Λ
0
+
Λ
s), while the permeance under RISC is only Λ
0 (see Table 1).Taking MPPUA as the exciting force, the stator vibration can be treated as the response. As indicated in Figure8, the stator vibration tendency at each harmonic frequency well follows the developing trend of MPPUA. Specifically, Figure 8(a) shows that the stator vibration in normal condition not only has each even harmonic component (primarily the 2nd and the 4th harmonics) but also includes each odd harmonic component (primarily the 1st, 3rd, and 5th harmonics). In theory, as analyzed previously, there should be only even harmonic components existing (primarily the 2nd harmonic). The extra odd harmonic components of the stator vibration are mainly transferred from the rotor vibration (the rotor and the stator both located on the basis; see Figure 3(a)) and caused by the initial asymmetry inside the generator. To study the essential effect of each kind of fault on the stator vibration, the vibration amplitudes of each harmonic in normal condition are treated as the null drifts of the experiment system, and the faulty vibration amplitudes are subtracted by these null drifts. For example, comparing with the normal condition, vibration amplitude at 2f for 0.1 mm, 0.2 mm, and 0.3 mm SAGE increases by 32.9% (0.886 mm/s), 50.5% (1.359 mm/s), and 70.9% (1.909 mm/s), respectively. This indicates that these increments of the vibration amplitude are the essential impact caused by the three SAGE fault conditions.To better show the relation between the input excitation force and the output vibration response, the line charts of MPPUA and the stator vibration at each frequency under different running conditions are illustrated in Figure9. It is shown that the developing tendency of the tested stator vibration amplitudes at each harmonic frequency generally accords with the changing trend of MPPUA. Meanwhile, it is also clear that as SAGE increases, both MPPUA and the vibration under CF have a larger value atf, 3f, and 4f but in the meantime have a smaller value at 2f than those under the single SAGE fault. However, as RISC develops, both MPPUA and the stator vibration will have a larger value under the CF condition than under the single RISC fault. These results are in good accordance with the conclusions obtained previously, confirming that both the FEM calculation and the experiment data match the previous analysis. In addition, this also indicates that the stator vibration response is consistent with the exciting MPPUA.Figure 9
Comparison between MPPUA and tested stator vibration for different conditions.
(a)
MPPUA when SAGE varies
(b)
Vibration when SAGE varies
(c)
MPPUA when RISC develops
(d)
Vibration when RISC develops


## 3.2.3. Fault Identification Criterion

Based on the theoretical analysis, the numerical FEM calculation, and the experiment study, it is found that the stator vibration characteristic varies under different faulty conditions. This can be employed to develop an identification criterion for the single and the composite faults composed of SAGE and RISC. More details can be found in Table3.Table 3
Fault identification criterion based on stator vibration characteristics.
Stator vibration characteristics
Performing condition
Having only soft 2nd harmonic vibrations
Normal condition
The vibration at 2f is increased, while the other components generally keep stable
SAGE exists
The vibration at 2f is decreased, but meanwhile vibrations at f, 3f, and 4fare increased
RISC exists
The vibration at 2f is firstly decreased and then increased; meanwhile, vibrations at f, 3f, and 4fare increased
CF exists


## 4. Conclusions

This paper investigates the stator vibration difference among SAGE, RISC, and the composite faults composed of SAGE and RISC. Based on the proposed theoretical analysis, the numerical FEM calculation, and the experimental study, primary conclusions can be generally drawn as follows:(1)
Normally, stator vibration has only the 2nd harmonic component in theory, while actually it also has the 1st harmonic component which is transferred from the rotor vibration. The occurrence of SAGE will increase the 2nd harmonic component.
(2)
As RISC and CF take place in the generator, extra stator vibrations atf, 2f, 3f, and 4f will be produced. As RISC develops, the 1st, 3rd, and the 4th harmonic components will be increased, while the 2nd harmonic component will be decreased.
(3)
In the case of CF, the increment of SAGE will raise the 1st, 2nd, 3rd, and the 4th harmonic components of the stator vibration at the same time, while under the single SAGE fault only the 2nd harmonic component will be increased.
(4)
As RISC develops, the stator vibration under CF atf, 2f, 3f, and 4f will have a larger intensity than under the single RISC fault. However, as SAGE increases, the stator vibration under CF will be more intensive atf, 3f, and 4f but meanwhile have weaker amplitude at 2f than under the single SAGE fault.Potentially, these sensitive conclusions can be applied to the practical online monitoring on the generators. Since it is very convenient to test the stator vibration with the industrial velocity sensors, further development of monitoring systems and utilities, which will be beneficial for the fault identification among SAGE, RISC, and the composite fault composed of SAGE and RISC, is probably to be carried out.



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*Source: 5971081-2016-10-16.xml*