JPH01295640A - Rotor for rotary electric machine - Google Patents

Rotor for rotary electric machine

Info

Publication number
JPH01295640A
JPH01295640A JP12391588A JP12391588A JPH01295640A JP H01295640 A JPH01295640 A JP H01295640A JP 12391588 A JP12391588 A JP 12391588A JP 12391588 A JP12391588 A JP 12391588A JP H01295640 A JPH01295640 A JP H01295640A
Authority
JP
Japan
Prior art keywords
rotor
vibration
shaft
torsional vibration
inherent
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP12391588A
Other languages
Japanese (ja)
Inventor
Yukihiko Kazao
幸彦 風尾
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Toshiba Corp
Original Assignee
Toshiba Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Toshiba Corp filed Critical Toshiba Corp
Priority to JP12391588A priority Critical patent/JPH01295640A/en
Publication of JPH01295640A publication Critical patent/JPH01295640A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To suppress torsional vibration of a rotor by equalizing the inherent vibration based on the torsional spring constant between an inertia disc fixed to the end of a rotor shaft and a rotor core to the inherent torsional vibration at rotor core section. CONSTITUTION:The rotor shaft of a rotor core 1 for large generator having axial length longer than the diameter is supported rotatably through bearings 4, 5. Then it is coupled through a coupling 2 arranged at the other end of the shaft to a turbine not shown. An inertia disc 3 is fixed to the other end of the shaft. Fixing position and the weight of the inertia disc 3 are set such that the inherent vibration based on the torsional spring constant of a vibration system comprising the shaft section 6 and the inertia disc 3 will be equal to the inherent torsional vibration at the section of the rotor core 1. By such arrangement, torsional vibration of the rotor is suppressed sufficiently even if the inherent torsional vibration at the rotor core section 1 matches to the magnetic exciting frequency, resulting in protection of turbine blade from damage.

Description

【発明の詳細な説明】 〔発明の目的〕 (産業上の利用分野) 本発明は回転電機の回転子の制振構造に係り、特に特定
のねじり振動を抑制できる回転電機の回転子構造に関す
る。
DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] (Industrial Application Field) The present invention relates to a vibration damping structure for a rotor of a rotating electrical machine, and particularly to a rotor structure for a rotating electrical machine that can suppress specific torsional vibrations.

(従来の技術) タービン発電機などの回転子は長い鉄心部分を有し、こ
の鉄心部分の両端が逆位相でねじれる振動が起こりやす
い、また通常運転状態においては固定子より系統電源周
波数(東日本においては5゜抛、西日本においては60
七)とその2倍の周波数の電磁加振力が回転子に作用し
、これにより回転子にはねじり振動が振動される。
(Prior art) The rotor of a turbine generator, etc. has a long iron core, and both ends of this iron core tend to vibrate and twist in opposite phases. is 5°, and in western Japan it is 60
7) and an electromagnetic excitation force with twice the frequency acts on the rotor, thereby causing torsional vibration in the rotor.

さて、固定子よりの電磁力の分布は一様であり、回転子
の鉄心部を含め鉄心中央より見て左右の慣性モーメント
が全く同じならば、鉄心両端が逆位相でねじれる振動モ
ードが励振されることはないが、現実には左右の慣性モ
ーメントは不均一になり電磁力による励振を受けること
になる。ただし。
Now, if the distribution of electromagnetic force from the stator is uniform, and if the left and right moments of inertia are exactly the same when viewed from the center of the core, including the rotor core, then a vibration mode in which both ends of the core twist in opposite phases will be excited. However, in reality, the moments of inertia on the left and right sides will be non-uniform and will be subject to excitation by electromagnetic force. however.

振動周波数(東日本においては50Hzと100七、西
日本においては6〇七と120H2)と鉄心部のねじり
振動の固有振動数が一致するかかなり近接しない限り、
問題はなかった。なお両者が一致した場合(共振)には
、そのねじり振動は拡大され機器に多大の影響を扱ぼす
ことになる。
Unless the vibration frequency (50Hz and 1007 in eastern Japan, 607 and 120H2 in western Japan) and the natural frequency of the torsional vibration of the iron core match or are very close to each other,
There were no problems. Note that when the two match (resonance), the torsional vibration is magnified and has a great influence on the equipment.

(発明が解決しようとする課題) 近年タービン発電機の容量の拡大に伴いその回転子の鉄
心部も長大化する傾向にあり、そのため前述の鉄心両端
が逆位相でねじれる振動モードの固有振動数が従来より
も低くなり機器によっては加振周波数にかなり近接した
り、場合によって一致する可能性が出て来た。万一共振
が起こると。
(Problem to be solved by the invention) In recent years, with the expansion of the capacity of turbine generators, the iron core of the rotor has also tended to become longer, and as a result, the natural frequency of the vibration mode in which both ends of the iron core are twisted in opposite phases has increased. It has become lower than before, and depending on the device, it may be quite close to the excitation frequency, or even coincide with it in some cases. In the unlikely event that resonance occurs.

鉄心部のねじり振動が拡大し、これがタービン側に伝達
されてタービン羽根を大きく振動させる。
The torsional vibration in the iron core expands and is transmitted to the turbine side, causing the turbine blades to vibrate greatly.

ここでタービン羽根の中に、その曲げ振動の固有振動数
が共振しているねじり振動の周波数に近いものがあると
、羽根の振動がさらに拡大され、致命的な破損に敗る。
If there is a turbine blade whose natural frequency of bending vibration is close to the frequency of the torsional vibration with which it resonates, the vibration of the blade will be further amplified, resulting in fatal damage.

発電所の公共性を考え合わせると、このような事態は何
としても回避しなくてはならない。
Considering the public nature of power plants, such a situation must be avoided at all costs.

そこで本発明の目的は、上述した問題点を解消し、回転
子鉄心部のねじり振動の固有振動数が電磁加振周波数に
一致したとしても1回転子のねじり振動を充分に抑制す
ることのできる回転電機の回転子を提供することにある
SUMMARY OF THE INVENTION Therefore, an object of the present invention is to solve the above-mentioned problems and to be able to sufficiently suppress torsional vibration of one rotor even if the natural frequency of torsional vibration of the rotor core matches the electromagnetic excitation frequency. Our objective is to provide rotors for rotating electric machines.

〔発明の構成〕[Structure of the invention]

(課題を解決するための手段) 上記目的を達成するため本発明の回転子は回転子上の鉄
心部具外の部分に慣性円板を設け1回転子鉄心端とこの
慣性円板間のねじりばね定数より成るねじり振動系の固
有振動数が回転子鉄心部の(作 用) 本発明の作用を第2図ないし第4図を用いて説明する。
(Means for Solving the Problems) In order to achieve the above object, the rotor of the present invention is provided with an inertia disk on a portion of the rotor outside the core component, and the torsion between the end of the rotor core and this inertia disk is The natural frequency of the torsional vibration system consisting of a spring constant is determined by the function of the rotor core.The function of the present invention will be explained with reference to FIGS. 2 to 4.

第2図はタービン発電機の回転子で、中央に鉄心部1を
有し、左端はタービンとのカップリング2、右端には慣
性円板3が取り付けられている。
FIG. 2 shows a rotor of a turbine generator, which has an iron core 1 in the center, a coupling 2 to the turbine at the left end, and an inertia disk 3 at the right end.

いま鉄心の両端が逆位相でねじれる振動モードとこれを
制振するための、本発明による作用を説明するため、第
3図の数学モデルを考える。図のJiとJ2はそれぞれ
鉄心部左右端の等偏集中慣性モーメント、には鉄心部の
ねじりばね定数、Jdは本発明による慣性円板の慣性モ
ーメント、kdは鉄心端より慣性円板までのシャフト部
が有するねじりばね定数である。さて鉄心郡全体には固
定子より周波数ω(ランフ2フ秒)の正弦波状の電磁加
振力によるトルク変動が作用すると考えると、第3図の
モデルの運動方程式は式■のようになる。
In order to explain the vibration mode in which both ends of the iron core are twisted in opposite phases and the action of the present invention for damping this vibration, consider the mathematical model shown in FIG. In the figure, Ji and J2 are the equally concentrated moments of inertia at the left and right ends of the core, respectively, are the torsional spring constants of the core, Jd is the moment of inertia of the disc of inertia according to the present invention, and kd is the shaft from the end of the core to the disc of inertia. is the torsional spring constant of the part. Now, assuming that torque fluctuations due to a sinusoidal electromagnetic excitation force of frequency ω (ramp 2 seconds) act on the entire iron core group from the stator, the equation of motion of the model in FIG. 3 becomes as shown in equation (2).

ただし、θ□、θ2.θdはそれぞれ集中慣性、Jx+
 Jay Jdの角変位、(・)は(・)の時間tによ
る2階微分を表わす、またT、、T、はJ、、J、に作
用するトルクである。
However, θ□, θ2. θd is concentrated inertia, Jx+
The angular displacement of Jay Jd, (·) represents the second derivative of (·) with respect to time t, and T,,T, is the torque acting on J,,J,.

説明を簡単にするため仮にJ、=J、=J、ω:=2に
/J、 Ja/J=αとおくと、式■の左辺より求まる
系の共振周波数比Ω=ω/ω。は、 Ω2=1+旦士ニジα2+2α    ■となる、ただ
し本発明によりkd/Jd=ω:となるようJdが決定
されているものとする。
To simplify the explanation, if J, = J, = J, ω: = 2 are set as /J, Ja/J = α, then the resonance frequency ratio of the system Ω = ω/ω is determined from the left side of equation (2). Ω2=1+Master Niji α2+2α (2) However, it is assumed that Jd is determined according to the present invention so that kd/Jd=ω:.

もし本発明によるJdがないもの(Jd=O)とすれば
α=Oとなり式■よりΩ2=1となる。
If it is assumed that there is no Jd according to the present invention (Jd=O), then α=O and Ω2=1 from equation (2).

すなわち、共振振動数ω=ω。(ω。:J、、J、とk
によって成る系の固有振動数に)になり、固定子よりの
励振周波数ωが系の固有振動数ω。に−致すると第4図
(a)に示す通り、系の角変位(θ、と02)の振幅が
極大となる。
That is, the resonant frequency ω=ω. (ω.: J,, J, and k
), and the excitation frequency ω from the stator is the natural frequency ω of the system. As shown in FIG. 4(a), the amplitude of the angular displacement (θ, 02) of the system becomes maximum.

ところが本発明による慣性円板Jdを取り付けることに
より第4図(b)に示す通りΩは式■より1+旦を境に
2つの共振周波数(すなわち1+量一14/α2+2α
 と1+!+IA/α2+2α を有し。
However, by attaching the inertia disk Jd according to the present invention, Ω becomes two resonant frequencies (i.e., 1 + quantity - 14/α2 + 2α
And 1+! +IA/α2+2α.

逆にΩ=1では極大とならない。Conversely, when Ω=1, there is no maximum.

すなわち本発明により、系のねじり固有振動数が固定子
よりの励振周波数に一致するような場合にも、第4図(
b)に示すごとく、共振を回避することができる。
That is, according to the present invention, even when the torsional natural frequency of the system matches the excitation frequency from the stator, the
As shown in b), resonance can be avoided.

(実施例) 以下、本発明の一実施例を図面を参照して説明する。(Example) Hereinafter, one embodiment of the present invention will be described with reference to the drawings.

第1図は本発明の一実施例であるタービン発電機回転子
で、中央部に鉄心1を有し、一端にはタービンとのカッ
プリング2、他端には慣性円板3を有している。なお回
転子は軸受4と5によって支えられているものとする図
中[=] で示した部分6は鉄心端と慣性円板間のシャ
フト部分で、このねじりばね定数kdと慣性円板3の慣
性モーメントJdとの間にJla/Ja =ω。なる関
係が成立するようJ8およびkdの値が決定されている
。ただしω。は回転子鉄心のねじり振動の固有振動数で
鉄心両端が逆位相でねじれるモードである。
FIG. 1 shows a turbine generator rotor according to an embodiment of the present invention, which has an iron core 1 in the center, a coupling 2 with a turbine at one end, and an inertia disk 3 at the other end. There is. It is assumed that the rotor is supported by bearings 4 and 5. In the figure, the part 6 indicated by [=] is the shaft part between the core end and the inertia disk, and this torsional spring constant kd and the inertia disk 3 are Between the moment of inertia Jd, Jla/Ja = ω. The values of J8 and kd are determined so that the following relationship holds true. However, ω. is the natural frequency of the torsional vibration of the rotor core, and is a mode in which both ends of the core twist in opposite phase.

第5図ないし第8図は本発明の他の実施例を示すもので
第5図は第3軸受けで支えられる継ぎシャフト8および
カップリングフランジ9の慣性モーメントがJdとなり
、シャフト部10のばね定数kdとともにJka/Ja
 ” (110となるよう構成されている。
5 to 8 show other embodiments of the present invention. In FIG. 5, the moment of inertia of the joint shaft 8 and the coupling flange 9 supported by the third bearing is Jd, and the spring constant of the shaft portion 10 is Jka/Ja with kd
” (It is configured to be 110.

第6図は発電機のカップリングフランジ2.タービン側
のフランジ11や、ターニング用ギヤ12を含めてこれ
らの慣性モーメントがJdeシャフト部13のねじりば
ね定数がkdで前述の関係が成立するよう構成されてい
る。
Figure 6 shows the coupling flange 2 of the generator. The moment of inertia of the flange 11 on the turbine side and the turning gear 12 is Jde, and the torsion spring constant of the shaft portion 13 is kd, so that the above-mentioned relationship is established.

第7図はエキサイタ14の慣性モーメントJdとシャフ
ト部15のばね定数kdの間に前述の関係を、第8図は
通風ファン用フランジ16の慣性モーメントJdとシャ
フト部17のばね定数kdの間と同様の関係が成立する
よう構成されている実施例である。
FIG. 7 shows the above-mentioned relationship between the moment of inertia Jd of the exciter 14 and the spring constant kd of the shaft portion 15, and FIG. 8 shows the relationship between the moment of inertia Jd of the ventilation fan flange 16 and the spring constant kd of the shaft portion 17. This is an example in which a similar relationship is established.

なお第8図においては、タービン側にある通風ファン用
フランジを用いて構成しても同様の効果がある。
In addition, in FIG. 8, the same effect can be obtained even if the configuration is made using a ventilation fan flange on the turbine side.

〔発明の効果〕〔Effect of the invention〕

以上の説明から明らかなように、本発明によれば回転電
機の回転子に回転子の特定のねじり振動の固有振動数と
等しい固有振動数になるよう慣性円板の慣性モーメント
とこの円板取付位置と鉄心端間のシャフトのばね定数を
構成することにより、たとえ固定子よりの電磁加振力に
よるトルク変動の周波数と鉄心のねじり振動の固有振動
数が一致しても、共振することはなく、タービン羽根と
の間に達成振動を生じて、タービン羽根に致命的な損傷
を与えることが回避できるなどの効果が得られる。
As is clear from the above description, according to the present invention, the moment of inertia of the inertia disk and the attachment of this disk to the rotor of a rotating electrical machine are set so that the rotor has a natural frequency equal to the natural frequency of a specific torsional vibration of the rotor. By configuring the spring constant of the shaft between the position and the core end, resonance will not occur even if the frequency of torque fluctuation due to electromagnetic excitation force from the stator matches the natural frequency of the torsional vibration of the core. Effects such as being able to avoid causing vibration between the turbine blade and the turbine blade and causing fatal damage to the turbine blade can be obtained.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明の一実施例による回転電機の回転子を示
す側面図、第2図ないし第4図は本発明1・・・回転子
鉄心、    2・・・カップリング、3・・・慣性円
板、    4・・・軸受。 5・・・軸受、      6・・・シャフト部、7・
・・第3軸受、     8・・・継ぎシャフト、9・
・・カップリングフランジ。 10・・・シャフト部、 11・・・タービン側カップリングフランジ、12・・
・ターニング用ギア、13・・・シャフト部、14・・
・エキサイタ、   15・・・シャフト部、16・・
・通風ファン用フランジ。 17・・・シャフト部 代理人 弁理士  則 近 憲 佑 同     第子丸   健 第1図 第2vA 第3図 ′。[戚数の 第4図
FIG. 1 is a side view showing a rotor of a rotating electric machine according to an embodiment of the present invention, and FIGS. 2 to 4 show the following according to the present invention: 1...rotor core, 2...coupling, 3... Inertia disk, 4...Bearing. 5... Bearing, 6... Shaft part, 7...
...Third bearing, 8...Joint shaft, 9.
...Coupling flange. 10... Shaft portion, 11... Turbine side coupling flange, 12...
・Turning gear, 13...Shaft part, 14...
・Exciter, 15...Shaft part, 16...
・Flange for ventilation fan. 17...Shaft Department Agent Patent Attorney Nori Ken Chika Yudo Ken Daishimaru Figure 1 Figure 2vA Figure 3'. [Figure 4 of relative numbers

Claims (1)

【特許請求の範囲】[Claims] 回転子上の鉄心部以外の部分に慣性円板を設け、回転子
鉄心端とこの慣性円板間のねじりばね定数より成るねじ
り振動系の固有振動数が回転子鉄心部のねじり振動の固
有振動数と一致するよう構成したことを特徴とする回転
電機の回転子。
An inertia disk is provided on a portion of the rotor other than the core, and the natural frequency of the torsional vibration system consisting of the torsional spring constant between the end of the rotor core and this inertia disk is the natural frequency of the torsional vibration of the rotor core. A rotor for a rotating electric machine, characterized in that the rotor is configured to match the number of rotors.
JP12391588A 1988-05-23 1988-05-23 Rotor for rotary electric machine Pending JPH01295640A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12391588A JPH01295640A (en) 1988-05-23 1988-05-23 Rotor for rotary electric machine

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12391588A JPH01295640A (en) 1988-05-23 1988-05-23 Rotor for rotary electric machine

Publications (1)

Publication Number Publication Date
JPH01295640A true JPH01295640A (en) 1989-11-29

Family

ID=14872494

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12391588A Pending JPH01295640A (en) 1988-05-23 1988-05-23 Rotor for rotary electric machine

Country Status (1)

Country Link
JP (1) JPH01295640A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20100108252A (en) * 2009-03-27 2010-10-06 제너럴 일렉트릭 캄파니 Tuning frequency of rotating body torsional mode by adding detuner

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20100108252A (en) * 2009-03-27 2010-10-06 제너럴 일렉트릭 캄파니 Tuning frequency of rotating body torsional mode by adding detuner
JP2010230166A (en) * 2009-03-27 2010-10-14 General Electric Co <Ge> Tuning frequency of rotating body torsional mode by adding detuner

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