Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JP6535208B2 - Structure identification device for vibration analysis model and identification method thereof - Google Patents
[go: Go Back, main page]

JP6535208B2 - Structure identification device for vibration analysis model and identification method thereof - Google Patents

Structure identification device for vibration analysis model and identification method thereof Download PDF

Info

Publication number
JP6535208B2
JP6535208B2 JP2015097479A JP2015097479A JP6535208B2 JP 6535208 B2 JP6535208 B2 JP 6535208B2 JP 2015097479 A JP2015097479 A JP 2015097479A JP 2015097479 A JP2015097479 A JP 2015097479A JP 6535208 B2 JP6535208 B2 JP 6535208B2
Authority
JP
Japan
Prior art keywords
vibration
vibration data
factor
measurement conditions
measurement
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.)
Active
Application number
JP2015097479A
Other languages
Japanese (ja)
Other versions
JP2016212016A (en
Inventor
神保 智彦
智彦 神保
日比野 良一
良一 日比野
山口 裕之
裕之 山口
大坪 秀顕
秀顕 大坪
稲川 智一
智一 稲川
芳男 浦上
芳男 浦上
伸二 加藤
伸二 加藤
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.)
Toyota Motor Corp
Toyota Central R&D Labs Inc
Original Assignee
Toyota Motor Corp
Toyota Central R&D Labs Inc
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 Toyota Motor Corp, Toyota Central R&D Labs Inc filed Critical Toyota Motor Corp
Priority to JP2015097479A priority Critical patent/JP6535208B2/en
Publication of JP2016212016A publication Critical patent/JP2016212016A/en
Application granted granted Critical
Publication of JP6535208B2 publication Critical patent/JP6535208B2/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Landscapes

  • Measurement Of Mechanical Vibrations Or Ultrasonic Waves (AREA)

Description

本発明は、複数の振動要素を有する振動系の解析モデルの構造同定を行う振動解析モデルの構造同定装置及びその同定方法に関する。   The present invention relates to a structural identification device of a vibration analysis model that performs structural identification of an analysis model of a vibration system having a plurality of vibration elements, and a method of identifying the same.

下記特許文献1のモデル同定装置では、鉄鋼の圧延プロセスにおける圧延荷重予測モデルに数式モデル同定を適用している。数式モデルの同定の際には、実績データを2グループに分類する分類パターンのうち、2グループ相互間における数式モデルの予測誤差の統計情報の差異が大きくなる分類パターンを決定し、決定した分類パターンでのグループ毎に数式モデルを同定する処理を、モデル予測精度が設定条件を満たすまで順次グループをさらに細分化しながら繰り返し、設定条件を満たしたときのパラメータをそのグループにおける数式モデルのパラメータとして設定する。分類パターンの決定は、まず平均値や標準偏差に基づいてグループ分類に用いるデータ項目を選択し、その中から情報量規範に基づいて採用する分類パターンを決定する。   In the model identification device of Patent Document 1 below, mathematical model identification is applied to a rolling load prediction model in a steel rolling process. In the identification of the mathematical expression model, among the classification patterns for classifying the actual data into two groups, the classification pattern in which the difference in statistical information of the prediction error of the mathematical expression model between the two groups is large is determined. The process of identifying a mathematical expression model for each group is repeated while further dividing the group sequentially until the model prediction accuracy satisfies the setting condition, and the parameter when the setting condition is satisfied is set as the parameter of the mathematical expression model in that group . In the determination of the classification pattern, first, the data item to be used for the group classification is selected based on the average value or the standard deviation, and the classification pattern to be adopted from them is determined based on the information amount standard.

また、下記特許文献2の振動解析装置では、振動系の複数箇所における振動データを取得し、各振動データをウェーブレット変換することで時間と周波数の関数である多次元ベクトルデータを生成し、多次元ベクトルデータを用いて因子解析(PARAFAC解析)を行うことで複数の独立したベクトルを生成する。複数の独立したベクトルは、振動の周波数的特徴と時間的特徴と空間的特徴を有する。   Moreover, in the vibration analysis device of the following patent document 2, multi-dimensional vector data which is a function of time and frequency is generated by acquiring vibration data at a plurality of locations of a vibration system and performing wavelet transform on each vibration data. By performing factor analysis (PARAFAC analysis) using vector data, multiple independent vectors are generated. The plurality of independent vectors have vibrational frequency characteristics, temporal characteristics and spatial characteristics.

特開2005−157788号公報JP 2005-157788 A 特開2010−48684号公報JP, 2010-48684, A 特開2004−280450号公報Unexamined-Japanese-Patent No. 2004-280450

特許文献1では、数式モデルを統計的に回帰する同定方法であるため、同定された数式モデルは物理的な意味を有さない。また、特許文献2では、振動の周波数的特徴と時間的特徴と空間的特徴を有する複数の独立したベクトルを因子解析により生成しているが、振動解析モデルの構造同定については示されておらず、振動解析モデルの低次元化についても考慮されていない。   In Patent Document 1, the identified mathematical expression model has no physical meaning because it is an identification method that statistically regresses the mathematical expression model. Further, in Patent Document 2, a plurality of independent vectors having frequency characteristics of vibration, temporal characteristics and spatial characteristics are generated by factor analysis, but structural identification of the vibration analysis model is not shown. Also, no consideration is given to the reduction of the vibration analysis model.

本発明は、物理的な意味を有し且つ低次元化された振動系の解析モデルの構造同定を行うことを目的とする。   An object of the present invention is to perform structural identification of an analytical model of a vibration system which has physical meaning and is reduced in dimension.

本発明に係る振動解析モデルの構造同定装置及びその同定方法は、上述した目的を達成するために以下の手段を採った。   The structure identification device for a vibration analysis model and the identification method according to the present invention employ the following means in order to achieve the above-mentioned object.

本発明に係る振動解析モデルの構造同定装置は、複数の振動要素を有する振動系の解析モデルの構造同定を行う振動解析モデル同定装置であって、振動系における振動計測対象とする振動要素及び振動計測方向のいずれか1つ以上が互いに異なる複数の計測条件での時系列振動データを取得する時系列振動データ取得部と、時系列振動データ取得部で取得された各時系列振動データを、時間及び周波数に対する振動データに変換する振動データ変換部と、振動データ変換部で変換された各振動データに対して所定の因子数で因子解析を行うことで、因子に対応する各計測条件の寄与度を算出する因子解析部と、振動データ変換部で変換された複数の計測条件での振動データにおいて、振動評価対象とする振動データと、それ以外の振動データと、因子解析部で算出された寄与度との関係に基づいて、振動評価対象以外の各計測条件に対応する重み係数を算出する重み係数算出部と、振動データ変換部で変換された複数の計測条件での振動データにおいて、振動評価対象を除くすべての計測条件について重み係数で重み付けした振動データを加算した総和と、振動評価対象を除く一部の計測条件について重み係数で重み付けした振動データを加算した総和との誤差を表す指標に基づいて計測条件を限定し、該限定した計測条件に基づいて解析モデルの構造同定を行う解析モデル同定部と、を備えることを要旨とする。   The structural identification device for a vibration analysis model according to the present invention is a vibration analysis model identification device for structural identification of an analysis model of a vibration system having a plurality of vibration elements, and the vibration element and vibration to be vibration measurement targets in the vibration system. A time-series vibration data acquisition unit that acquires time-series vibration data under a plurality of measurement conditions in which one or more of the measurement directions are different from one another, and each time-series vibration data acquired by the time-series vibration data acquisition unit The factor of each measurement condition corresponding to the factor by performing factor analysis on each piece of vibration data converted by the vibration data converter that converts vibration data with respect to frequency and frequency, and each vibration data converted by the vibration data converter In the vibration data under a plurality of measurement conditions converted by the factor analysis unit that calculates the vibration data and the vibration data conversion unit, the vibration data to be evaluated for vibration and the other vibration data A weight coefficient calculation unit that calculates a weight coefficient corresponding to each measurement condition other than the vibration evaluation target based on the relationship between the contribution degree calculated by the factor analysis unit, and a plurality of measurements converted by the vibration data conversion unit In the vibration data under the conditions, the sum of the vibration data weighted by the weighting factor for all measurement conditions excluding the vibration evaluation target and the vibration data weighted with the weighting factor for some measurement conditions excluding the vibration evaluation target are added The present invention is characterized in that the measurement condition is limited based on an index representing an error with the total sum, and an analysis model identification unit that performs structure identification of the analysis model based on the limited measurement condition is provided.

本発明の一態様では、解析モデル同定部は、前記指標を算出する際に、因子解析部で算出された寄与度に基づいて前記一部の計測条件を選択することが好適である。   In one aspect of the present invention, when the analysis model identification unit calculates the index, it is preferable that the partial measurement condition be selected based on the degree of contribution calculated by the factor analysis unit.

本発明の一態様では、因子解析部は、振動データ変換部で変換された各振動データに対して複数の因子数で因子解析を行うことで、各因子毎に時間及び周波数に対する振動データを算出し、該算出した各因子毎の振動データに基づいて因子を選択し、解析モデル同定部は、前記指標を算出する際に、因子解析部で選択された因子に対応する寄与度に基づいて前記一部の計測条件を選択することが好適である。   In one aspect of the present invention, the factor analysis unit performs factor analysis on each vibration data converted by the vibration data conversion unit with a plurality of factor numbers to calculate vibration data for time and frequency for each factor. The factor is selected based on the calculated vibration data for each factor, and the analysis model identification unit calculates the index based on the degree of contribution corresponding to the factor selected by the factor analysis unit. It is preferable to select some of the measurement conditions.

本発明の一態様では、因子解析部は、各因子毎の振動データにおける振幅の変動度合いに基づいて因子を選択することが好適である。   In one aspect of the present invention, it is preferable that the factor analysis unit select a factor based on the degree of fluctuation of the amplitude in the vibration data for each factor.

また、本発明に係る振動解析モデルの構造同定方法は、複数の振動要素を有する振動系の解析モデルの構造同定を行う振動解析モデル同定方法であって、振動系における振動計測対象とする振動要素及び振動計測方向のいずれか1つ以上が互いに異なる複数の計測条件での時系列振動データを取得する時系列振動データ取得処理と、時系列振動データ取得処理で取得された各時系列振動データを、時間及び周波数に対する振動データに変換する振動データ変換処理と、振動データ変換処理で変換された各振動データに対して所定の因子数で因子解析を行うことで、因子に対応する各計測条件の寄与度を算出する因子解析処理と、振動データ変換処理で変換された複数の計測条件での振動データにおいて、振動評価対象とする振動データと、それ以外の振動データと、因子解析処理で算出された寄与度との関係に基づいて、振動評価対象以外の各計測条件に対応する重み係数を算出する重み係数算出処理と、振動データ変換処理で変換された複数の計測条件での振動データにおいて、振動評価対象を除くすべての計測条件について重み係数で重み付けした振動データを加算した総和と、振動評価対象を除く一部の計測条件について重み係数で重み付けした振動データを加算した総和との誤差を表す指標に基づいて計測条件を限定し、該限定した計測条件に基づいて解析モデルの構造同定を行う解析モデル同定処理と、を含むことを要旨とする。   The structure identification method of a vibration analysis model according to the present invention is a vibration analysis model identification method for performing structure identification of an analysis model of a vibration system having a plurality of vibration elements, the vibration element to be a vibration measurement target in the vibration system. Time series vibration data acquisition processing for acquiring time series vibration data under a plurality of measurement conditions in which one or more of the vibration measurement directions are different from each other, and each time series vibration data acquired in the time series vibration data acquisition processing Vibration data conversion processing for converting to vibration data with respect to time and frequency, and performing factor analysis on each vibration data converted by the vibration data conversion processing with a predetermined number of factors, for each measurement condition corresponding to the factor In the factor analysis processing for calculating the degree of contribution, and in the vibration data under a plurality of measurement conditions converted by the vibration data conversion processing, vibration data to be evaluated for vibration, and Based on the relationship between vibration data other than vibration data and contribution degree calculated by factor analysis processing, weight coefficient calculation processing that calculates the weight coefficient corresponding to each measurement condition other than vibration evaluation target, and conversion by vibration data conversion processing In the vibration data under the plurality of measurement conditions, the sum of the vibration data weighted by the weighting factor for all the measurement conditions except for the vibration evaluation target and the weight coefficient for some measurement conditions except the vibration evaluation target Abstract: A measurement condition is limited based on an index representing an error with a sum of added vibration data, and analysis model identification processing for identifying a structure of an analysis model based on the limited measurement condition is included. .

本発明によれば、振動評価対象を除くすべての計測条件について重み係数で重み付けした振動データを加算した総和と、振動評価対象を除く一部の計測条件について重み係数で重み付けした振動データを加算した総和との誤差を表す指標に基づいて限定した計測条件により解析モデルの構造同定を行うことで、物理的な意味を有し且つ低次元化された振動系の解析モデルの構造同定を行うことができる。   According to the present invention, the sum obtained by adding the vibration data weighted by the weighting factor for all measurement conditions excluding the vibration evaluation target and the vibration data weighted by the weighting factor for some measurement conditions except the vibration evaluation target are added The structural identification of an analytical model of a vibration system having a physical meaning and reduced in dimension can be performed by performing structural identification of the analytical model under limited measurement conditions based on an index representing an error with the sum. it can.

本発明の実施形態に係る振動解析モデルの構造同定装置の適用対象となる車両の概略構成を示す図である。BRIEF DESCRIPTION OF THE DRAWINGS It is a figure which shows schematic structure of the vehicle which becomes application object of the structure identification apparatus of the vibration analysis model which concerns on embodiment of this invention. 車両のパワートレインブロックの概略構成を示す図である。It is a figure which shows schematic structure of the powertrain block of a vehicle. 車両のパワートレインブロックの概略構成を示す図である。It is a figure which shows schematic structure of the powertrain block of a vehicle. 本発明の実施形態に係る振動解析モデルの構造同定装置の概略構成を示す図である。It is a figure showing a schematic structure of a structure identification device of a vibration analysis model concerning an embodiment of the present invention. ウェーブレット変換により得られる3次元配列X_の一例を示す図である。It is a figure which shows an example of three-dimensional array X_ obtained by wavelet transformation. 3次元配列X_をPARAFAC解析により行列A,B,Cに分解する処理を説明する図である。It is a figure explaining the process to decompose | disassemble 3-dimensional array X_ into matrix A, B, C by PARAFAC analysis. PARAFAC解析により得られた因子の基底ウェーブレットの一例を示す図である。It is a figure which shows an example of the basis wavelet of the factor obtained by PARAFAC analysis. 選択された因子fに対応する各計測条件(k=1〜K)の寄与度c1f〜cKfの一例を示す図である。Is a diagram illustrating an example of a contribution c 1f to c Kf of each measurement conditions corresponding to the selected factor f (k = 1~K). ランキングrに対する指標Erの関係を計算した結果の一例を示す図である。It is a figure which shows an example of the result of having calculated the relationship of the parameter | index E r with respect to ranking r. 振動解析モデルの一例を示す図である。It is a figure which shows an example of a vibration analysis model.

以下、本発明を実施するための形態(以下実施形態という)を図面に従って説明する。   Hereinafter, modes for carrying out the present invention (hereinafter referred to as embodiments) will be described according to the drawings.

図1〜3は本発明の実施形態に係る振動解析モデルの構造同定装置の適用対象となる車両10の概略構成を示す図であり、図4は本発明の実施形態に係る振動解析モデルの構造同定装置の概略構成を示す図である。図1は本実施形態における車両10全体の概略構成を示し、図2,3はパワートレインブロック12の概略構成を示す。振動系としての車両10は、複数の振動要素として車体(ばね上要素)11とパワートレインブロック12とばね下要素15を含む。パワートレインブロック12はエンジン13及び変速機14を含んで構成され、ばね下要素15は駆動輪18及びロワアーム19を含んで構成される。エンジン13は変速機14に連結され、変速機14は駆動輪18に連結されている。車両10の実稼働(実走行)時に、エンジン13はトルク(回転力)を加振力として発生し、エンジン13と変速機14間でトルクが伝達され、変速機14と駆動輪18間でトルクが伝達される。パワートレインブロック12はマウント16を介して車体11に支持されており、マウント16を介してパワートレインブロック12と車体11間で力が伝達される。ばね下要素15はサスペンションブッシュ17を介して車体11に支持されており、サスペンションブッシュ17を介してばね下要素15と車体11間で力が伝達される。   1 to 3 are diagrams showing a schematic configuration of a vehicle 10 to which a structural identification apparatus for a vibration analysis model according to an embodiment of the present invention is applied. FIG. 4 is a structure of a vibration analysis model according to an embodiment of the present invention It is a figure which shows schematic structure of an identification apparatus. FIG. 1 shows a schematic configuration of the entire vehicle 10 in the present embodiment, and FIGS. 2 and 3 show a schematic configuration of a power train block 12. A vehicle 10 as a vibration system includes a vehicle body (sprung element) 11, a power train block 12, and an unsprung element 15 as a plurality of vibration elements. The powertrain block 12 is configured to include the engine 13 and the transmission 14, and the unsprung element 15 is configured to include the drive wheel 18 and the lower arm 19. The engine 13 is coupled to a transmission 14, and the transmission 14 is coupled to a drive wheel 18. During actual operation (actual traveling) of the vehicle 10, the engine 13 generates torque (rotational force) as an excitation force, torque is transmitted between the engine 13 and the transmission 14, and torque between the transmission 14 and the driving wheel 18 Is transmitted. The power train block 12 is supported by the vehicle body 11 via the mount 16, and power is transmitted between the power train block 12 and the vehicle body 11 via the mount 16. The unsprung element 15 is supported by the vehicle body 11 via the suspension bush 17, and the force is transmitted between the unsprung element 15 and the vehicle body 11 via the suspension bush 17.

ここで、車両前後方向(車両進行方向)をx軸、車両左右方向をy軸、車両上下方向をz軸とする、互いに直交するxyz3次元座標系を車両10に規定する。パワートレインブロック12は、x方向重心軸まわりに回転振動(ロール振動)可能であり、y方向重心軸まわりに回転振動(ピッチ振動)可能であり、z方向重心軸まわりに回転振動(ヨー振動)可能である。さらに、パワートレインブロック12は、x方向に並進振動可能であり、y方向に並進振動可能であり、z方向に並進振動可能である。同様に、ばね下要素15も、x方向重心軸まわりに回転振動(ロール振動)可能であり、y方向重心軸まわりに回転振動(ピッチ振動)可能であり、z方向重心軸まわりに回転振動(ヨー振動)可能である。さらに、ばね下要素15も、x方向に並進振動可能であり、y方向に並進振動可能であり、z方向に並進振動可能である。車体11は、x方向に並進振動可能である。ここでは、パワートレインブロック12及びばね下要素15は、6自由度の剛体運動をする質点であるものとして考える。以下の実施形態では、加振源であるエンジン13のトルク振動に対して車体11のフロアのx方向並進振動を評価する車両10の振動解析モデルの構造同定を行う例について説明する。   Here, an xyz three-dimensional coordinate system orthogonal to each other is defined in the vehicle 10 with the vehicle longitudinal direction (vehicle traveling direction) as the x axis, the vehicle lateral direction as the y axis, and the vehicle vertical direction as the z axis. The power train block 12 is capable of rotational vibration (roll vibration) around the x-direction center of gravity axis, rotational vibration (pitch vibration) around the y-direction center of gravity axis, and rotational vibration (yaw vibration) around the z-direction center of gravity axis It is possible. Furthermore, the powertrain block 12 is capable of translational vibration in the x direction, translational vibration in the y direction, and translational vibration in the z direction. Similarly, the unsprung element 15 is also capable of rotational vibration (roll vibration) around the x-direction center of gravity axis, rotational vibration (pitch vibration) around the y-direction center of gravity axis, and rotational vibration around the z-direction center of gravity axis Yaw vibration) is possible. Furthermore, the unsprung element 15 is also capable of translational vibration in the x direction, translational vibration in the y direction, and translational vibration in the z direction. The vehicle body 11 can translate and vibrate in the x direction. Here, the powertrain block 12 and the unsprung element 15 are considered to be mass points with rigid motion with six degrees of freedom. In the following embodiment, an example will be described in which the structure identification of the vibration analysis model of the vehicle 10 is performed in which the x-direction translational vibration of the floor of the vehicle body 11 is evaluated with respect to the torque vibration of the engine 13 which is a vibration source.

車両10の実走行時における振動計測対象であるパワートレインブロック12の並進振動及び回転振動を計測するために、図2,3に示すように、各々がx方向並進加速度とy方向並進加速度とz方向並進加速度を検出する複数(3つ)の3軸加速度センサ22−1,22−2,22−3がパワートレインブロック12に付設されている。図2,3の例では、3軸加速度センサ22−1と3軸加速度センサ22−2はy方向に互いに距離lp1+lp2をおいた状態でパワートレインブロック12に設置され、3軸加速度センサ22−1と3軸加速度センサ22−3はy方向に互いに距離lp1+lp3をおいた状態でパワートレインブロック12に設置されている。3軸加速度センサ22−1と3軸加速度センサ22−2とでx方向位置及びz方向位置は互いに等しく、3軸加速度センサ22−1,22−2と3軸加速度センサ22−3は、x方向に互いに距離dp1+dp3をおき、z方向に互いに距離hp1+hp3をおいた状態で、パワートレインブロック12に設置されている。 As shown in FIGS. 2 and 3, in order to measure the translational vibration and rotational vibration of the powertrain block 12 which is the vibration measurement target during actual traveling of the vehicle 10, each has x-direction translational acceleration and y-direction translational acceleration and z. A plurality of (three) three-axis acceleration sensors 22-1, 22-2, 22-3 for detecting the direction translational acceleration are attached to the power train block 12. In the example of FIGS. 2 and 3, the three-axis acceleration sensor 22-1 and the three-axis acceleration sensor 22-2 are installed in the power train block 12 with a distance l p1 + l p2 in the y direction. The 22-1 and 3-axis acceleration sensors 22-3 are installed in the power train block 12 with a distance l p1 + l p3 in the y direction. The x-direction position and the z-direction position of the 3-axis acceleration sensor 22-1 and the 3-axis acceleration sensor 22-2 are equal to each other, and the 3-axis acceleration sensors 22-1 and 22-2 and the 3-axis acceleration sensor 22-3 are x The power train block 12 is installed at a distance d p1 + d p3 in the direction and in a direction h p1 + h p3 in the z direction.

パワートレインブロック12において、x方向重心軸まわりの回転角加速度d2θpx/dt2は以下の(1)式で表され、y方向重心軸まわりの回転角加速度d2θpy/dt2は以下の(2)式で表され、z方向重心軸まわりの回転角加速度d2θpz/dt2は以下の(3)式で表される。そして、重心点でのx方向並進加速度d2p/dt2は以下の(4)式で表され、重心点でのy方向並進加速度d2p/dt2は以下の(5)式で表され、重心点でのz方向並進加速度d2p/dt2は以下の(6)式で表される。(1)〜(6)式において、d2p1/dt2は3軸加速度センサ22−1の付設箇所でのz方向並進加速度、d2p3/dt2は3軸加速度センサ22−3の付設箇所でのz方向並進加速度、d2p1/dt2は3軸加速度センサ22−1の付設箇所でのx方向並進加速度、d2p2/dt2は3軸加速度センサ22−2の付設箇所でのx方向並進加速度、d2p3/dt2は3軸加速度センサ22−3の付設箇所でのx方向並進加速度、d2p1/dt2は3軸加速度センサ22−1の付設箇所でのy方向並進加速度である。そして、hp1はパワートレインブロック12の重心点と3軸加速度センサ22−1,22−2の付設箇所とのz方向距離、dp1はパワートレインブロック12の重心点と3軸加速度センサ22−1,22−2の付設箇所とのx方向距離、lp1はパワートレインブロック12の重心点と3軸加速度センサ22−1の付設箇所とのy方向距離である。 In the power train block 12, the rotational angular acceleration d 2 θ px / dt 2 about the x-direction center of gravity axis is expressed by the following equation (1), and the rotational angular acceleration d 2 θ py / dt 2 about the y-direction central axis of gravity The rotational angular acceleration d 2 θ pz / dt 2 about the z-direction center of gravity axis is expressed by the following expression (2). The x-direction translational acceleration d 2 x p / dt 2 at the center of gravity is expressed by the following equation (4), and the y-direction translational acceleration d 2 y p / dt 2 at the center of gravity is the following equation (5) The z-direction translational acceleration d 2 x p / dt 2 at the center of gravity is expressed by the following equation (6). In equations (1) to (6), d 2 z p 1 / dt 2 is the z-direction translational acceleration at the location where the 3-axis acceleration sensor 22-1 is attached, and d 2 z p 3 / dt 2 is the 3-axis acceleration sensor 22-3 Z-direction translational acceleration at the installation site, d 2 x p 1 / dt 2 is the x-axis translational acceleration at the installation site of the 3-axis acceleration sensor 22-1, d 2 x p 2 / dt 2 is the 3-axis acceleration sensor 22-2 X-direction translational acceleration at the attachment point of the sensor, d 2 x p 3 / dt 2 is the x-direction translational acceleration at the attachment point of the 3-axis acceleration sensor 22-3, and d 2 y p 1 / dt 2 is the 3-axis acceleration sensor 22-1 Y-direction translational acceleration at the attachment point of Further, h p1 is the z-direction distance between the center of gravity of the power train block 12 and the attachment point of the three-axis acceleration sensor 22-1, 22-2 and d p1 is the center of gravity of the power train block 12 and the three-axis acceleration sensor 22- The x-direction distance from the attachment point of 1, 22-2 and l p1 is the y-direction distance between the center of gravity of the power train block 12 and the attachment point of the three-axis acceleration sensor 22-1.

2θpx/dt2=(d2p3/dt2−d2p1/dt2)/(lp1+lp3) (1)
2θpy/dt2=(d2p1/dt2−d2p3/dt2)/(hp1+hp3) (2)
2θpz/dt2=(d2p1/dt2−d2p2/dt2)/(lp1+lp2) (3)
2p/dt2=d2p1/dt2
−hp1×d2θpy/dt2−lp1×d2θpz/dt2 (4)
2p/dt2=d2p1/dt2
−dp1×d2θpz/dt2+hp1×d2θpx/dt2 (5)
2p/dt2=d2p1/dt2
+dp1×d2θpy/dt2+lp1×d2θpx/dt2 (6)
d 2 θ px / dt 2 = (d 2 z p 3 / dt 2 −d 2 z p 1 / dt 2 ) / (l p 1 + l p 3 ) (1)
d 2 θ py / dt 2 = (d 2 x p 1 / dt 2 −d 2 x p 3 / dt 2 ) / (h p 1 + h p 3 ) (2)
d 2 θ pz / dt 2 = (d 2 x p 1 / dt 2 −d 2 x p 2 / dt 2 ) / (l p 1 + l p 2 ) (3)
d 2 x p / dt 2 = d 2 x p 1 / dt 2
−h p1 × d 2 θ py / dt 2 −l p 1 × d 2 θ pz / dt 2 (4)
d 2 y p / dt 2 = d 2 y p1 / dt 2
−d p 1 × d 2 θ pz / dt 2 + h p 1 × d 2 θ px / dt 2 (5)
d 2 z p / dt 2 = d 2 z p 1 / dt 2
+ D p 1 x d 2 θ py / dt 2 + l p 1 x d 2 θ px / dt 2 (6)

同様に、車両10の実走行時における振動計測対象であるばね下要素15(ロワアーム19)の並進振動及び回転振動を計測するために、各々がx方向並進加速度とy方向並進加速度とz方向並進加速度を検出する複数(3つ)の3軸加速度センサ25−1,25−2,25−3がばね下要素15に付設されている。3軸加速度センサ25−1と3軸加速度センサ25−2はy方向に互いに距離ls1+ls2をおいた状態でばね下要素15に設置され、3軸加速度センサ25−1と3軸加速度センサ25−3はy方向に互いに距離ls1+ls3をおいた状態でばね下要素15に設置されている。3軸加速度センサ25−1と3軸加速度センサ25−2とでx方向位置及びz方向位置は互いに等しく、3軸加速度センサ25−1,25−2と3軸加速度センサ25−3は、x方向に互いに距離ds1+ds3をおき、z方向に互いに距離hs1+hs3をおいた状態で、ばね下要素15に設置されている。 Similarly, in order to measure the translational vibration and rotational vibration of the unsprung element 15 (lower arm 19), which is the vibration measurement target during actual traveling of the vehicle 10, each has x-direction translational acceleration, y-direction translational acceleration and z-direction translation A plurality of (three) three-axis acceleration sensors 25-1, 25-2, 25-3 for detecting acceleration are attached to the unsprung element 15. The triaxial acceleration sensor 25-1 and the triaxial acceleration sensor 25-2 are installed on the unsprung element 15 with the distance l s1 + l s2 mutually set in the y direction, and the triaxial acceleration sensor 25-1 and the triaxial acceleration sensor 25-3 are installed on the unsprung element 15 with a distance l s1 + l s3 to each other in the y direction. The x-direction position and z-direction position of the 3-axis acceleration sensor 25-1 and the 3-axis acceleration sensor 25-2 are equal to each other, and the 3-axis acceleration sensor 25-1, 25-2 and the 3-axis acceleration sensor 25-3 are x It is installed in the unsprung element 15 in a state in which the distance d s1 + d s3 is mutually spaced in the direction and the distance h s1 + h s3 is mutually spaced in the z direction.

ばね下要素15(ロワアーム19)において、x方向重心軸まわりの回転角加速度d2θsx/dt2は以下の(7)式で表され、y方向重心軸まわりの回転角加速度d2θsy/dt2は以下の(8)式で表され、z方向重心軸まわりの回転角加速度d2θsz/dt2は以下の(9)式で表される。そして、重心点でのx方向並進加速度d2s/dt2は以下の(10)式で表され、重心点でのy方向並進加速度d2s/dt2は以下の(11)式で表され、重心点でのz方向並進加速度d2s/dt2は以下の(12)式で表される。(7)〜(12)式において、d2s1/dt2は3軸加速度センサ25−1の付設箇所でのz方向並進加速度、d2s3/dt2は3軸加速度センサ25−3の付設箇所でのz方向並進加速度、d2s1/dt2は3軸加速度センサ25−1の付設箇所でのx方向並進加速度、d2s2/dt2は3軸加速度センサ25−2の付設箇所でのx方向並進加速度、d2s3/dt2は3軸加速度センサ25−3の付設箇所でのx方向並進加速度、d2s1/dt2は3軸加速度センサ25−1の付設箇所でのy方向並進加速度である。そして、hs1はばね下要素15の重心点と3軸加速度センサ25−1,25−2の付設箇所とのz方向距離、ds1はばね下要素15の重心点と3軸加速度センサ25−1,25−2の付設箇所とのx方向距離、ls1はばね下要素15の重心点と3軸加速度センサ25−1の付設箇所とのy方向距離である。 In the unsprung element 15 (lower arm 19), the rotational angular acceleration d 2 θ sx / dt 2 around the center of gravity in the x direction is expressed by the following equation (7), and the rotational angular acceleration d 2 θ sy around the center of gravity in the y direction / Dt 2 is expressed by the following equation (8), and the rotational angular acceleration d 2 θ sz / dt 2 about the z-axis center of gravity is expressed by the following equation (9). The x-direction translational acceleration d 2 x s / dt 2 at the center of gravity is expressed by the following equation (10), and the y-direction translational acceleration d 2 y s / dt 2 at the center of gravity is the following equation (11) The z-direction translational acceleration d 2 x s / dt 2 at the center of gravity is expressed by the following equation (12). (7) - (12) In the equation, d 2 z s1 / dt 2 is the z-direction translational acceleration in attached position of three-axis acceleration sensor 25-1, d 2 z s3 / dt 2 is the three-axis acceleration sensor 25-3 z-direction translational acceleration in attached position of, d 2 x s1 / dt 2 is the x-direction translational acceleration in attached position of three-axis acceleration sensor 25-1, d 2 x s2 / dt 2 is the three-axis acceleration sensor 25-2 x-direction translational acceleration, d 2 x s3 / dt 2 is the x-direction translational acceleration in attached position of three-axis acceleration sensor 25-3, d 2 y s1 / dt 2 is 3-axis acceleration sensor 25-1 at the attached portion Y-direction translational acceleration at the attachment point of And h s1 is the z-direction distance between the center of gravity of the unsprung element 15 and the attachment point of the three-axis acceleration sensor 25-1, 25-2, d s1 is the center of gravity of the unsprung element 15 and the three-axis acceleration sensor 25 The x-direction distance from the attachment site of 1, 25-2 and l s1 is the y-direction distance between the center of gravity of the unsprung element 15 and the attachment site of the three-axis acceleration sensor 25-1.

2θsx/dt2=(d2s3/dt2−d2s1/dt2)/(ls1+ls3) (7)
2θsy/dt2=(d2s1/dt2−d2s3/dt2)/(hs1+hs3) (8)
2θsz/dt2=(d2s1/dt2−d2s2/dt2)/(ls1+ls2) (9)
2s/dt2=d2s1/dt2
−hs1×d2θsy/dt2−ls1×d2θsz/dt2 (10)
2s/dt2=d2s1/dt2
−ds1×d2θsz/dt2+hs1×d2θsx/dt2 (11)
2s/dt2=d2s1/dt2
+ds1×d2θsy/dt2+ls1×d2θsx/dt2 (12)
d 2 θ sx / dt 2 = (d 2 z s3 / dt 2 -d 2 z s1 / dt 2) / (l s1 + l s3) (7)
d 2 θ sy / dt 2 = (d 2 x s1 / dt 2 -d 2 x s3 / dt 2) / (h s1 + h s3) (8)
d 2 θ sz / dt 2 = (d 2 x s1 / dt 2 -d 2 x s2 / dt 2) / (l s1 + l s2) (9)
d 2 x s / dt 2 = d 2 x s1 / dt 2
-H s1 × d 2 θ sy / dt 2 -l s1 × d 2 θ sz / dt 2 (10)
d 2 y s / dt 2 = d 2 y s1 / dt 2
−d s1 × d 2 θ sz / dt 2 + h s1 × d 2 θ sx / dt 2 (11)
d 2 z s / dt 2 = d 2 z s1 / dt 2
+ D s1 × d 2 θ sy / dt 2 + l s1 × d 2 θ sx / dt 2 (12)

車両10の実走行時における振動計測対象である駆動輪18の回転振動を計測するために、駆動輪18の角速度dθw/dtを検出する角速度センサ28が駆動輪18に付設されている。また、車両10の実走行時における振動評価対象である車体11のフロアの並進振動を計測するために、車体11のフロアのx方向並進加速度d2v/dt2を検出する加速度センサ21が車体11のフロアに付設されている。車両10の実走行時に各センサ21,22−1,22−2,22−3,25−1,25−2,25−3,28で検出された時系列信号は、振動解析装置70に入力される。振動解析装置70は、車両10の振動解析を行うための解析モデルの構造同定を行う。 An angular velocity sensor 28 for detecting an angular velocity dθ w / dt of the drive wheel 18 is attached to the drive wheel 18 in order to measure rotational vibration of the drive wheel 18 which is an object of vibration measurement during actual traveling of the vehicle 10. Further, in order to measure the translational vibration of the floor of the vehicle body 11 which is an object of vibration evaluation during actual traveling of the vehicle 10, the acceleration sensor 21 detects x-direction translational acceleration d 2 x v / dt 2 of the floor of the vehicle body 11. It is attached to the floor of the vehicle body 11. The time series signals detected by the sensors 21, 22-1, 22-2, 22-3, 25-1, 25-2, 25-3, 28 when the vehicle 10 is actually traveling are input to the vibration analysis device 70. Be done. The vibration analysis device 70 performs structure identification of an analysis model for analyzing the vibration of the vehicle 10.

振動解析装置70の機能ブロック図の一例を図4に示す。振動解析装置70は、CPUを中心としたコンピュータとして構成可能であり、コンピュータを以下に説明する時系列振動データ取得部71、設定定数記憶装置72、振動データ変換部73、因子解析部74、重み係数算出部75、及び解析モデル同定部76として機能させる。   An example of a functional block diagram of the vibration analysis device 70 is shown in FIG. The vibration analysis device 70 can be configured as a computer with a CPU as a center, and the computer will be described below. The time-series vibration data acquisition unit 71, the setting constant storage device 72, the vibration data conversion unit 73, the factor analysis unit 74, the weights It functions as a coefficient calculation unit 75 and an analysis model identification unit 76.

振動解析装置70において、設定定数記憶装置72には、前述の距離lp1+lp2,lp1+lp3,hp1+hp3,lp1,hp1,dp1,ls1+ls2,ls1+ls3,hs1+hs3,ls1,hs1,ds1が記憶されている。時系列振動データ取得部71には、各センサ21,22−1,22−2,22−3,25−1,25−2,25−3,28で検出された時系列信号が入力される。時系列振動データ取得部71は、車両10(振動系)における振動計測対象とする振動要素及び振動計測方向のいずれか1つ以上が互いに異なる複数の計測条件での時系列振動データを取得する。ここでは、複数の計測条件での時系列振動データとして、車体11のフロアのx方向並進加速度d2v/dt2と、駆動輪18の回転角加速度d2θw/dt2と、パワートレインブロック12の並進加速度d2p/dt2,d2p/dt2,d2p/dt2及び回転角加速度d2θpx/dt2,d2θpy/dt2,d2θpz/dt2と、ばね下要素15(ロワアーム19)の並進加速度d2s/dt2,d2s/dt2,d2s/dt2及び回転角加速度d2θsx/dt2,d2θsy/dt2,d2θsz/dt2が取得され、14通りの計測条件での時系列振動加速度が取得される。 In vibration analysis device 70, the set constant storage device 72, the distance of the aforementioned l p1 + l p2, l p1 + l p3, h p1 + h p3, l p1, h p1, d p1, l s1 + l s2, l s1 + l s3 , H s1 + h s3 , l s1 , h s1 , d s1 are stored. The time-series vibration data acquisition unit 71 receives time-series signals detected by the sensors 21, 22-2, 22-2, 22-3, 25-1, 25-2, 25-3, 28. . The time-series vibration data acquisition unit 71 acquires time-series vibration data under a plurality of measurement conditions in which one or more of the vibration element to be subjected to vibration measurement in the vehicle 10 (vibration system) and the vibration measurement direction are different. Here, the x-direction translational acceleration d 2 x v / dt 2 of the floor of the vehicle body 11, the rotational angular acceleration d 2 θ w / dt 2 of the drive wheel 18, and power as time-series vibration data under a plurality of measurement conditions Translational acceleration of the train block 12 d 2 x p / dt 2 , d 2 y p / dt 2 , d 2 z p / dt 2 and rotational angular acceleration d 2 θ px / dt 2 , d 2 θ py / dt 2 , d and 2 θ pz / dt 2, translational acceleration d 2 x s / dt 2, d 2 y s / dt 2, d 2 z s / dt 2 and the rotational angular acceleration d 2 theta unsprung element 15 (lower arm 19) sx / Dt 2 , d 2 θ sy / dt 2 , d 2 θ sz / dt 2 are acquired, and time-series vibrational accelerations under 14 measurement conditions are acquired.

車体11のフロアのx方向並進加速度d2v/dt2は、加速度センサ21の検出信号から取得される。駆動輪18の回転角加速度d2θw/dt2は、角速度センサ28で検出された角速度dθw/dtを微分することで取得される。パワートレインブロック12において、x方向重心軸まわりの回転角加速度d2θpx/dt2は、3軸加速度センサ22−3,22−1で検出されたz方向並進加速度の差d2p3/dt2−d2p1/dt2に基づいて(1)式により算出され、y方向重心軸まわりの回転角加速度d2θpy/dt2は、3軸加速度センサ22−1,22−3で検出されたx方向並進加速度の差d2p1/dt2−d2p3/dt2に基づいて(2)式により算出され、z方向重心軸まわりの回転角加速度d2θpz/dt2は、3軸加速度センサ22−1,22−2で検出されたx方向並進加速度の差d2p1/dt2−d2p2/dt2に基づいて(3)式により算出される。そして、重心点でのx方向並進加速度d2p/dt2は、回転角加速度d2θpy/dt2,d2θpz/dt2と3軸加速度センサ22−1で検出されたx方向並進加速度d2p1/dt2とに基づいて(4)式により算出され、重心点でのy方向並進加速度d2p/dt2は、回転角加速度d2θpz/dt2,d2θpx/dt2と3軸加速度センサ22−1で検出されたy方向並進加速度d2p1/dt2とに基づいて(5)式により算出され、重心点でのz方向並進加速度d2p/dt2は、回転角加速度d2θpy/dt2,d2θpx/dt2と3軸加速度センサ22−1で検出されたz方向並進加速度d2p1/dt2とに基づいて(6)式により算出される。 The x-direction translational acceleration d 2 x v / dt 2 of the floor of the vehicle body 11 is obtained from the detection signal of the acceleration sensor 21. The rotational angular acceleration d 2 θ w / dt 2 of the drive wheel 18 is obtained by differentiating the angular velocity dθ w / dt detected by the angular velocity sensor 28. In the power train block 12, the rotational angular acceleration d 2 θ px / dt 2 about the x-direction center of gravity axis is the difference d 2 z p 3 / of the z-direction translational acceleration detected by the three-axis acceleration sensor 22-3, 22-1. Based on dt 2 −d 2 z p 1 / dt 2 , the rotational angular acceleration d 2 θ py / dt 2 about the y-direction center of gravity axis is calculated using the three-axis acceleration sensors 22-1 and 22-3. Based on the difference d 2 x p 1 / dt 2 −d 2 x p 3 / dt 2 of the x-direction translational acceleration detected by the equation (2), and the rotational angular acceleration d 2 θ pz / dt 2 is calculated by the equation (3) based on the difference d 2 x p 1 / dt 2 -d 2 x p 2 / dt 2 of the x-direction translational acceleration detected by the three-axis acceleration sensors 22-1 and 22-2 Ru. The x-direction translational acceleration d 2 x p / dt 2 at the center of gravity is x detected by the rotational angular acceleration d 2 θ py / dt 2 , d 2 θ pz / dt 2 and the 3-axis acceleration sensor 22-1 Based on the direction translational acceleration d 2 x p 1 / dt 2 , the y-direction translational acceleration d 2 y p / dt 2 at the center of gravity is calculated by the equation (4), and the rotational angular acceleration d 2 θ pz / dt 2 , Calculated by equation (5) based on d 2 θ px / dt 2 and y-direction translational acceleration d 2 y p 1 / dt 2 detected by the 3-axis acceleration sensor 22-1, z-direction translational acceleration at the center of gravity d 2 x p / dt 2 is the rotational angular acceleration d 2 θ py / dt 2 , d 2 θ px / dt 2 and z-axis translational acceleration detected by the 3-axis acceleration sensor 22-1 d 2 z p 1 / dt 2 And is calculated by equation (6).

同様に、ばね下要素15(ロワアーム19)において、x方向重心軸まわりの回転角加速度d2θsx/dt2は、3軸加速度センサ25−3,25−1で検出されたz方向並進加速度の差d2s3/dt2−d2s1/dt2に基づいて(7)式により算出され、y方向重心軸まわりの回転角加速度d2θsy/dt2は、3軸加速度センサ25−1,25−3で検出されたx方向並進加速度の差d2s1/dt2−d2s3/dt2に基づいて(8)式により算出され、z方向重心軸まわりの回転角加速度d2θsz/dt2は、3軸加速度センサ25−1,25−2で検出されたx方向並進加速度の差d2s1/dt2−d2s2/dt2に基づいて(9)式により算出される。そして、重心点でのx方向並進加速度d2s/dt2は、回転角加速度d2θsy/dt2,d2θsz/dt2と3軸加速度センサ25−1で検出されたx方向並進加速度d2s1/dt2とに基づいて(10)式により算出され、重心点でのy方向並進加速度d2s/dt2は、回転角加速度d2θsz/dt2,d2θsx/dt2と3軸加速度センサ25−1で検出されたy方向並進加速度d2s1/dt2とに基づいて(11)式により算出され、重心点でのz方向並進加速度d2s/dt2は、回転角加速度d2θsy/dt2,d2θsx/dt2と3軸加速度センサ25−1で検出されたz方向並進加速度d2s1/dt2とに基づいて(12)式により算出される。 Similarly, in the unsprung element 15 (lower arm 19), the rotational angular acceleration d 2 θ sx / dt 2 about the x-direction center of gravity axis is the z-direction translational acceleration detected by the three-axis acceleration sensor 25-3, 25-1. It is based of the difference d 2 z s3 / dt 2 -d 2 z s1 / dt 2 is calculated by equation (7), the rotational angular acceleration d 2 θ sy / dt 2 about the y-direction center of gravity axis, three-axis acceleration sensor based on the difference d 2 x s1 / dt 2 -d 2 x s3 / dt 2 of the detected x-direction translational acceleration in 25-1,25-3 calculated by equation (8), the rotation around the z-direction central axis angular acceleration d 2 θ sz / dt 2, based on 3 different x-direction translational acceleration detected by the axis acceleration sensor 25-1,25-2 d 2 x s1 / dt 2 -d 2 x s2 / dt 2 It is calculated by the equation (9). The x-direction translational acceleration d 2 x s / dt 2 at the center of gravity is x detected by the rotational angular acceleration d 2 θ sy / dt 2 , d 2 θ sz / dt 2 and the 3-axis acceleration sensor 25-1 is calculated by on the basis of the direction translational acceleration d 2 x s1 / dt 2 ( 10) equation, y-direction translational acceleration d 2 y s / dt 2 in the center of gravity, the angular acceleration d 2 θ sz / dt 2, based on the d 2 θ sx / dt 2 and 3-axis acceleration sensor 25 - 1 y-direction translational acceleration detected by d 2 y s1 / dt 2 is calculated by the equation (11), z-direction translational acceleration of the center of gravity point d 2 x s / dt 2, the rotation angular acceleration d 2 θ sy / dt 2, d 2 θ sx / dt 2 and 3 axis z-direction translational acceleration detected by the acceleration sensor 25-1 d 2 z s1 / dt 2 And calculated based on Eq. (12).

なお、x方向重心軸まわりの回転角速度とy方向重心軸まわりの回転角速度とz方向重心軸まわりの回転角速度を検出する3軸角速度センサをパワートレインブロック12やばね下要素15に設置し、3軸角速度センサの検出信号を微分することでパワートレインブロック12やばね下要素15の重心軸まわりの回転角加速度を取得することも可能である。また、x方向並進加速度とy方向並進加速度とz方向並進加速度を検出する3軸加速度センサをパワートレインブロック12やばね下要素15の重心点に直接設置可能な場合は、3軸加速度センサの検出信号からパワートレインブロック12やばね下要素15の重心点での並進加速度を取得することが可能である。   Note that a three-axis angular velocity sensor that detects the rotational angular velocity around the x-axis, y-axis, and the z-axis is installed in the powertrain block 12 or the unsprung element 15, 3 It is also possible to acquire the rotational angular acceleration around the center of gravity axis of the power train block 12 or the unsprung element 15 by differentiating the detection signal of the axial angular velocity sensor. If a 3-axis acceleration sensor that detects x-direction translational acceleration, y-direction translational acceleration, and z-direction translational acceleration can be installed directly at the center of gravity of powertrain block 12 or unsprung element 15, detection of the 3-axis acceleration sensor It is possible to obtain the translational acceleration at the center of gravity of the powertrain block 12 or the unsprung element 15 from the signal.

振動データ変換部73は、時系列振動データ取得部71で取得された各時系列振動データを時間周波数解析することで、時間及び周波数に対する振動データに変換する。ここでは、時系列振動データ取得部71で取得された各時系列振動データに対してウェーブレット(Wavelet)変換を施すことで、各時系列振動データを時間及び周波数に対する振動データに変換する。つまり、車体11のフロアのx方向並進加速度d2v/dt2と、駆動輪18の回転角加速度d2θw/dt2と、パワートレインブロック12の並進加速度d2p/dt2,d2p/dt2,d2p/dt2及び回転角加速度d2θpx/dt2,d2θpy/dt2,d2θpz/dt2と、ばね下要素15(ロワアーム19)の並進加速度d2s/dt2,d2s/dt2,d2s/dt2及び回転角加速度d2θsx/dt2,d2θsy/dt2,d2θsz/dt2が、ウェーブレット変換によって、時間及び周波数に対する振動加速度に変換される。これによって、図5に示すように、時間及び周波数に対する振動加速度の関係を表す行列Xk(kは1〜Kの整数、Kは計測条件の数で本実施形態では14通り)が各計測条件毎に得られ、時間と周波数と計測条件(計測箇所及び方向)に対する振動加速度の関係を表す3次元配列X_が得られる。ただし、図及び数式では、3次元配列X_を、Xの下に_(アンダーバー)を付して表す(他の3次元配列についても同様)。なお、ウェーブレット変換自体は公知であるため詳細な説明を省略する。 The vibration data conversion unit 73 performs time-frequency analysis on each time-series vibration data acquired by the time-series vibration data acquisition unit 71 to convert it into vibration data with respect to time and frequency. Here, wavelet transformation is performed on each of the time-series vibration data acquired by the time-series vibration data acquisition unit 71 to convert each of the time-series vibration data into vibration data with respect to time and frequency. That is, the x-direction translational acceleration d 2 x v / dt 2 of the floor of the vehicle body 11, the rotational angular acceleration d 2 θ w / dt 2 of the drive wheel 18, and the translational acceleration d 2 x p / dt 2 of the powertrain block 12 , D 2 y p / dt 2 , d 2 z p / dt 2 and rotational angular acceleration d 2 θ px / dt 2 , d 2 θ py / dt 2 , d 2 θ pz / dt 2 and the unsprung element 15 ( Translational acceleration d 2 x s / dt 2 , d 2 y s / dt 2 , d 2 z s / dt 2 and rotational angular acceleration d 2 θ sx / dt 2 , d 2 θ sy / dt 2 , d 2 θ sz / dt 2 is converted to vibrational acceleration with respect to time and frequency by wavelet transform. Thus, as shown in FIG. 5, a matrix X k (k is an integer from 1 to K, K is the number of measurement conditions and 14 in this embodiment) representing the relationship of vibration acceleration to time and frequency is each measurement condition A three-dimensional array X_ is obtained which is obtained for each time and which represents the relationship between vibration acceleration with respect to time, frequency, and measurement conditions (measurement location and direction). However, in the figures and formulas, the three-dimensional array X_ is represented by _ (under bar) below X (the same applies to other three-dimensional arrays). Note that the wavelet transform itself is known and thus the detailed description is omitted.

因子解析部74は、振動データ変換部73でウェーブレット変換された各振動データ(3次元配列X_)に対して所定の因子数で因子解析(PARAFAC解析)を行う。PARAFAC解析では、図6に示すように3次元配列X_を行列A,B,Cに分解して近似して表すことができ、3次元配列X_を2次元に行列化した行列Xは、以下の(13)式で近似して表すことができる。   The factor analysis unit 74 performs factor analysis (PARAFAC analysis) on each vibration data (three-dimensional array X_) wavelet-transformed by the vibration data conversion unit 73 with a predetermined number of factors. In PARAFAC analysis, as shown in FIG. 6, the three-dimensional array X_ can be expressed by being decomposed into matrices A, B, and C, and can be expressed. The matrix X obtained by matrixing the three-dimensional array X_ into two dimensions is It can be approximated and expressed by equation (13).

(13)式において、Tは転置を表す(以下の他式も同様)。行列Hは、対角に1、その他が0の3次元配列H_(図6参照)を2次元に行列化した行列である。行列Aは、周波数と因子に関わるI行F列(I,Fは2以上の整数)の行列であり、以下の(14)式に示すようにi行目f列目(iは1〜Iの整数、fは1〜Fの整数)の要素をaifとすると、行(i)が周波数に対応し、列(f)が因子に対応する。行列Bは、時間と因子に関わるJ行F列(Jは2以上の整数)の行列であり、以下の(15)式に示すようにj行目f列目(jは1〜Jの整数)の要素をbjfとすると、行(j)が時間に対応し、列(f)が因子に対応する。行列Cは、計測条件(計測箇所及び方向)と因子に関わるK行F列の行列であり、以下の(16)式に示すようにk行目f列目の要素をckfとすると、行(k)が計測条件に対応し、列(f)が因子に対応する。Iは周波数のサンプル点数、Jは時間のサンプル点数、Fは因子数である。3次元配列X_のi,j,kの要素X_ijkは、以下の(17)式で近似して表される。(17)式は、(13)式を書き換えたものである。 In Formula (13), T represents transposition (the following other formulas are also the same). The matrix H is a matrix obtained by two-dimensionally matrixing a three-dimensional array H_ (see FIG. 6) in which one is diagonally zero and the other is zero. The matrix A is a matrix of I rows and F columns (I and F are integers of 2 or more) related to the frequency and the factor, and the i-th row and the f-th column (i is 1 to I) as shown in the following equation (14) When an element of an integer of f and an integer of 1 to F is a if , row (i) corresponds to frequency and column (f) corresponds to a factor. The matrix B is a matrix of J rows and F columns (J is an integer of 2 or more) related to time and factors, and the j-th row and f-th column (j is an integer of 1 to J) as shown in the following equation (15) If the element of b) is b jf , row (j) corresponds to time and column (f) corresponds to a factor. The matrix C is a matrix of K rows and F columns relating to measurement conditions (measurement points and directions) and factors, and assuming that the element of the k th row and the f th column is c k f as shown in the following equation (16) (K) corresponds to the measurement condition, and column (f) corresponds to the factor. I is the number of frequency sample points, J is the number of time sample points, and F is the number of factors. I 3D array X_, j, elements X_ ijk of k is expressed by approximation by the following equation (17). The equation (17) is a rewrite of the equation (13).

因子解析部74は、3次元配列X_に対して複数の因子数でPARAFAC解析を行うことで、(13)式((17)式)をほぼ満たす行列A,B,Cを算出する。PARAFAC解析により行列A,B,Cを算出する処理自体は公知であるため詳細な説明を省略する。そして、因子解析部74は、各因子(f=1〜F)毎に周波数(i)及び時間(j)に対するaif×bjfの関係を算出することで、各因子毎に周波数及び時間に対する振動データを取得する。 The factor analysis unit 74 calculates the matrices A, B, and C substantially satisfying the equation (13) (the equation (17)) by performing the PARAFAC analysis on the three-dimensional array X_ with a plurality of factor numbers. Since the process itself which calculates the matrices A, B, and C by PARAFAC analysis is known, detailed description is omitted. Then, the factor analysis unit 74 calculates the relationship of a if × b jf to the frequency (i) and the time (j) for each factor (f = 1 to F) to obtain the frequency and time for each factor. Acquire vibration data.

各因子(f=1〜F)毎に周波数(i)及び時間(j)に対するaif×bjfの関係を算出することで得られた因子の基底ウェーブレットの一例を図7に示す。PARAFAC解析の際には、因子数F=5とし、図7(a)は、因子f=1での周波数及び時間に対するai1×bj1の関係を示し、図7(b)は、因子f=2での周波数及び時間に対するai2×bj2の関係を示し、図7(c)は、因子f=3での周波数及び時間に対するai3×bj3の関係を示し、図7(d)は、因子f=4での周波数及び時間に対するai4×bj4の関係を示し、図7(e)は、因子f=5での周波数及び時間に対するai5×bj5の関係を示す。図7(a)に示すように、因子f=1では、4Hzの周波数で振動の振幅が大きくなり、4Hzの振動の振幅が時間に対して大きく変動する過渡振動となる。同様に、図7(c)に示すように、因子f=3でも、11Hzの周波数で振動の振幅が大きくなり、11Hzの振動の振幅が時間に対して大きく変動する過渡振動となり、図7(e)に示すように、因子f=5でも、16Hzの周波数で振動の振幅が大きくなり、16Hzの振動の振幅が時間に対して大きく変動する過渡振動となる。一方、図7(b)に示すように、因子f=2では、6Hzの周波数で振動の振幅が大きくなるが、6Hzの振動の振幅が時間に対してほとんど変動しない定常振動となる。同様に、図7(d)に示すように、因子f=4でも、12Hzの周波数で振動の振幅が大きくなるが、12Hzの振動の振幅が時間に対してほとんど変動しない定常振動となる。 An example of the basis wavelet of the factor obtained by calculating the relationship of a if × b jf to the frequency (i) and the time (j) for each factor (f = 1 to F) is shown in FIG. In PARAFAC analysis, the number of factors is F = 5, and FIG. 7A shows the relationship of a i1 × b j1 to the frequency and time at a factor of f = 1, and FIG. = indicates the relationship between a i2 × b j2 with respect to frequency and time at 2, FIG. 7 (c) shows the relationship between a i3 × b j3 respect to frequency and time of a factor f = 3, FIG. 7 (d) Shows the relationship of a i4 × b j4 to the frequency and time at a factor f = 4, and FIG. 7 (e) shows the relationship of a i5 × b j5 to the frequency and time at a factor f = 5. As shown in FIG. 7A, when the factor f = 1, the amplitude of the vibration becomes large at a frequency of 4 Hz, and the amplitude of the 4 Hz vibration becomes a transient vibration that largely fluctuates with respect to time. Similarly, as shown in FIG. 7C, even with the factor f = 3, the amplitude of the vibration becomes large at a frequency of 11 Hz, and the amplitude of the vibration of 11 Hz becomes a transient vibration with a large fluctuation with time. As shown in e), even with the factor f = 5, the amplitude of the vibration becomes large at the frequency of 16 Hz, and the amplitude of the 16 Hz vibration becomes a transient vibration that largely fluctuates with respect to time. On the other hand, as shown in FIG. 7B, in the case of the factor f = 2, the amplitude of the vibration becomes large at a frequency of 6 Hz, but the vibration of 6 Hz becomes a steady vibration hardly fluctuating with time. Similarly, as shown in FIG. 7 (d), even with the factor f = 4, the amplitude of the vibration increases at a frequency of 12 Hz, but the amplitude of the 12 Hz vibration becomes a steady vibration that hardly varies with time.

因子解析部74は、各因子に対応する振動データに基づいて因子を選択する。ここでは、各因子(f=1〜F)に対応する振動データ(aif×bjf)の振幅の変動度合いに基づいて因子(f)が選択され、aif×bjfの振幅の変動度合いが所定量より大きい過渡振動となる因子(f)が選択される。図7の例では、定常振動となる因子f=2,4は選択されずに、過渡振動となる因子f=1,3,5が選択される。 The factor analysis unit 74 selects a factor based on vibration data corresponding to each factor. Here, the factor (f) is selected based on the fluctuation degree of the amplitude of the vibration data (a if × b jf ) corresponding to each factor (f = 1 to F), and the fluctuation degree of the amplitude of a if × b jf Is selected as a factor (f) which causes a transient vibration larger than a predetermined amount. In the example of FIG. 7, the factor f = 1, 2, 3 which is a transient vibration is selected without selecting the factor f = 2, 4 which is a steady state vibration.

PARAFAC解析により行列Cを算出することで、各因子毎に各計測条件の寄与度を算出することができ、行列Cのf列目の各要素c1f〜cKfが、因子(f)に対応する各計測条件(k=1〜K)の寄与度となる。選択された因子f=1に対応する各計測条件(k=1〜K)の寄与度c11〜cK1を図8(a)に示し、選択された因子f=3に対応する各計測条件(k=1〜K)の寄与度c13〜cK3を図8(b)に示し、選択された因子f=5に対応する各計測条件(k=1〜K)の寄与度c15〜cK5を図8(c)に示す。図8の例では、K=14であり、k=1が車体11のフロアのx方向並進加速度VE(X)に対応し、k=2が駆動輪18の回転角加速度WH(Rot)に対応する。そして、k=3,4,5,6,7,8が、ばね下要素15(ロワアーム19)における重心点でのx方向並進加速度LA(X)、y方向並進加速度LA(Y)、z方向並進加速度LA(Z)、x方向重心軸まわりの回転角加速度LA(Roll)、y方向重心軸まわりの回転角加速度LA(Pitch)、z方向重心軸まわりの回転角加速度LA(Yaw)にそれぞれ対応する。そして、k=9,10,11,12,13,14が、パワートレインブロック12における重心点でのx方向並進加速度PB(X)、y方向並進加速度PB(Y)、z方向並進加速度PB(Z)、x方向重心軸まわりの回転角加速度PB(Roll)、y方向重心軸まわりの回転角加速度PB(Pitch)、z方向重心軸まわりの回転角加速度PB(Yaw)にそれぞれ対応する。 By calculating the matrix C by PARAFAC analysis, the degree of contribution of each measurement condition can be calculated for each factor, and the elements c 1f to c Kf of the f th column of the matrix C correspond to the factor (f) The degree of contribution of each measurement condition (k = 1 to K). The degree of contribution c 11 to c K1 of each measurement condition (k = 1 to K) corresponding to the selected factor f = 1 is shown in FIG. 8A, and each measurement condition corresponding to the selected factor f = 3 The degree of contribution c 13 to c K 3 of (k = 1 to K ) is shown in FIG. 8B, and the degree of contribution c 15 of each measurement condition (k = 1 to K) corresponding to the selected factor f = 5 c K5 is shown in FIG. 8 (c). In the example of FIG. 8, K = 14, k = 1 corresponds to the x-direction translational acceleration VE (X) of the floor of the vehicle body 11, and k = 2 corresponds to the rotational angular acceleration WH (Rot) of the drive wheel 18 Do. Then, k = 3, 4, 5, 6, 7, 8 indicate the x-direction translational acceleration LA (X), y-direction translational acceleration LA (Y) at the center of gravity of the unsprung element 15 (lower arm 19), z-direction Translational acceleration LA (Z), Rotational angular acceleration LA (Roll) around the x-axis center of gravity, Rotational angular acceleration LA (Pitch) around the y-axis central axis, Rotational acceleration LA (Yaw) around the z-axis central axis It corresponds. Then, k = 9, 10, 11, 12, 13, and 14 represent the x-direction translational acceleration PB (X), the y-direction translational acceleration PB (Y), and the z-direction translational acceleration PB (Y) at the center of gravity in the powertrain block 12. Z), rotational angular acceleration PB (Roll) around the x-direction center of gravity axis, rotational angular acceleration PB (Pitch) around the y-direction central axis, and rotational angular acceleration PB (Yaw) around the z-direction central axis.

(17)式を以下の(18)式のように書き換える。行列Xkは、計測条件(k)において、ウェーブレット変換後の周波数(i)及び時間(j)に対する振動加速度の関係を表すI行J列の行列である。行列Mfは、因子(f)において、周波数(i)及び時間(j)に対するaif×bjf(図7の縦軸の値)の関係を表すI行J列の行列であり、以下の(19)式で表される。(19)式において、afは行列Aのf列目に対応するベクトル((14)式参照)であり、bfは行列Bのf列目に対応するベクトル((15)式参照)である。 The equation (17) is rewritten as the following equation (18). The matrix X k is a matrix of I rows and J columns representing the relationship of the vibration acceleration to the frequency (i) and time (j) after wavelet transform in the measurement condition (k). The matrix M f is a matrix of I rows and J columns representing the relationship of a if × b jf (the value of the vertical axis in FIG. 7) to the frequency (i) and time (j) in the factor (f). It is expressed by the equation (19). In equation (19), a f is a vector corresponding to the f-th column of matrix A (see equation (14)) and b f is a vector corresponding to f-th row of matrix B (see equation (15)) is there.

行列Xk,Mfの各要素を縦ベクトルに並べ換えて転置をとると横ベクトルvec(Xk)T,vec(Mf)Tとなり、(18)式は以下の(20)式のようになる。(20)式から以下の(21)式が得られる。 If each element of the matrices X k and M f is rearranged into a vertical vector and transposed, then the horizontal vectors vec (X k ) T and vec (M f ) T are obtained , and equation (18) is given by equation (20) below Become. The following equation (21) is obtained from the equation (20).

重み係数算出部75は、振動データ変換部73でウェーブレット変換された複数の計測条件での振動データX1〜XKにおいて、振動評価対象とする振動データ(本実施形態では車体11のフロアのx方向並進加速度)X1と、それ以外の振動データX2〜XKと、因子解析部74で算出された寄与度Cとの関係に基づいて、振動評価対象以外の各計測条件(k=2〜K)に対応する重み係数d2〜dKを算出する。(21)式を、振動評価対象とする振動データX1と、それ以外の振動データX2〜XKとに分けると、以下の(22)、(23)式が得られる。(22)、(23)式からvec(M1)T〜vec(MF)Tを消去すると、以下の(24)式が得られる。(24)式において、横ベクトルDは、横ベクトルC1と行列C2に基づく以下の(25)式で表される。つまり、(24)式は、振動評価対象とする振動データX1と、それ以外の振動データX2〜XKと、各因子に対応する各計測条件の寄与度Cとの関係式を表す。重み係数d2〜dKは、横ベクトルDの要素であり、横ベクトルC1と行列C2(寄与度C)に基づいて(25)式により算出される。 The weight coefficient calculation unit 75 calculates vibration data to be evaluated for vibration (in this embodiment, x of the floor of the vehicle body 11 in the vibration data X 1 to X K under a plurality of measurement conditions wavelet-transformed by the vibration data conversion unit 73). Based on the relationship between the direction translational acceleration) X 1 and the other vibration data X 2 to X K and the contribution degree C calculated by the factor analysis unit 74, each measurement condition other than the vibration evaluation target (k = 2 Weight coefficients d 2 to d K corresponding to to K) are calculated. If Formula (21) is divided into vibration data X 1 to be subjected to vibration evaluation and other vibration data X 2 to X K , the following Formulas (22) and (23) are obtained. If vec (M 1 ) T to vec (M F ) T are eliminated from the equations (22) and (23), the following equation (24) is obtained. In equation (24), the lateral vector D is expressed by the following equation (25) based on the lateral vector C 1 and the matrix C 2 . That is, (24) represents the vibration data X 1 to the vibration evaluated, otherwise the vibration data X 2 to X K of the relationship between the contribution C of each measurement conditions corresponding to each factor. The weighting factors d 2 to d K are elements of the horizontal vector D, and are calculated by equation (25) based on the horizontal vector C 1 and the matrix C 2 (degree of contribution C).

以下の(26)式に示すように、(24)式の右辺をyと定義する。yは、振動評価対象を除くすべての計測条件(k=2〜K)について、dk×vec(Xk)Tを加算した総和、つまり重み係数dkで重み付けした振動データXkを加算した総和を表す。また、以下の(27)式に示すように、振動評価対象を除く一部の計測条件について重み係数dkで重み付けした振動データXk(dk×vec(Xk)T)を加算した総和をy^rと定義する。ただし、数式では、y^rを、yrの上に^(ハット)を付して表す。 As shown in the following equation (26), the right side of the equation (24) is defined as y. y for all measurement conditions except for vibration evaluated (k = 2~K), the sum obtained by adding the d k × vec (X k) T, i.e. the sum of the vibration data X k weighted by weighting coefficients d k Represents the sum. Further, as shown in the following equation (27), a sum obtained by adding vibration data X k (d k × ve c (X k ) T ) weighted by the weighting coefficient d k for a part of measurement conditions excluding the vibration evaluation target Define y ^ r . However, in the formula, y ^ r is represented by adding ^ (hat) on y r .

解析モデル同定部76は、振動データ変換部73でウェーブレット変換された複数の計測条件での振動データX1〜XKにおいて、振動評価対象を除くすべての計測条件(k=2〜K)について重み係数dkで重み付けした振動データXkを加算した総和yと、振動評価対象を除く一部の計測条件について重み係数dkで重み付けした振動データXkを加算した総和y^rとの誤差を表す指標Erに基づいて、車両10の振動解析モデルで考慮する計測条件を限定する。総和yは(26)式により算出され、総和y^rは(27)式により算出される。yとy^rとの誤差を表す指標Erとしては、例えば以下の(28)式を用いることが可能である。ただし、振動評価対象である車体11のフロアのx方向並進加速度VE(X)(k=1)、及び加振源であるエンジン13のトルクにより駆動される駆動輪18の回転角加速度WH(Rot)(k=2)については、振動解析モデルで考慮する計測条件に含めるものとする。 The analysis model identification unit 76 weights all of the measurement conditions (k = 2 to K) except the vibration evaluation target in the vibration data X 1 to X K under a plurality of measurement conditions wavelet-transformed by the vibration data conversion unit 73. the sum y obtained by adding the vibration data X k weighted by coefficients d k, the error between the sum y ^ r obtained by adding the vibration data X k weighted by weighting coefficients d k for some measurement conditions, except for vibration evaluation The measurement conditions to be considered in the vibration analysis model of the vehicle 10 are limited based on the index E r to be represented. The total sum y is calculated by the equation (26), and the total sum ^ r is calculated by the equation (27). For example, the following equation (28) can be used as the index E r representing the error between y and y r . However, the x-direction translational acceleration VE (X) (k = 1) of the floor of the vehicle body 11 that is the vibration evaluation target, and the rotational angular acceleration WH (Rot) of the drive wheel 18 driven by the torque of the engine 13 that is the vibration source. ) (K = 2) is included in the measurement conditions considered in the vibration analysis model.

解析モデル同定部76での総和y^rの算出に用いる一部の計測条件は、因子解析部74で算出された各計測条件の寄与度ckfに基づいて選択される。より具体的には、総和y^rの算出に用いる一部の計測条件は、図8に示すような、因子解析部74で選択された因子f=1,3,5に対応する寄与度ckfに基づいて選択され、例えば各因子(f=1,3,5)毎に、計測条件(k)が寄与度ckfの絶対値の大きい順にランキング付けされて選択される。ただし、振動解析モデルで考慮する計測条件に含める駆動輪18の回転角加速度WH(Rot)(k=2)については、総和y^rの算出に用いる一部の計測条件に含めるものとする。そのため、k=3〜Kの計測条件のうち寄与度ckfの絶対値が大きい順に計測条件(k)が各因子(f=1,3,5)毎に選択される。 A part of measurement conditions used to calculate the total sum ^ r in the analysis model identification unit 76 is selected based on the degree of contribution c kf of each measurement condition calculated in the factor analysis unit 74. More specifically, a part of the measurement conditions used to calculate the total sum ^ r is the degree of contribution c corresponding to the factor f = 1, 3, 5 selected by the factor analysis unit 74 as shown in FIG. It is selected based on kf , and for example, for each factor (f = 1, 3, 5), the measurement condition (k) is selected by ranking in descending order of the absolute value of the degree of contribution c kf . However, the rotational angular acceleration WH (Rot) (k = 2) of the drive wheel 18 included in the measurement conditions considered in the vibration analysis model is included in some of the measurement conditions used for calculating the total sum y r . Therefore, among the measurement conditions of k = 3 to K, the measurement condition (k) is selected for each factor (f = 1, 3, 5) in the descending order of the absolute value of the degree of contribution c kf .

図8の例では、因子f=1に対応する計測条件(k=3〜K)の寄与度ck1の絶対値、及び因子f=3に対応する計測条件(k=3〜K)の寄与度ck3の絶対値は、パワートレインブロック12のy方向重心軸まわりの回転角加速度PB(Pitch)(k=13)が最も大きく、因子f=5に対応する計測条件(k=3〜K)の寄与度ck5の絶対値は、ばね下要素15(ロワアーム19)の重心点でのx方向並進加速度LA(X)(k=3)が最も大きい。そこで、ランキングr=1では、一部の計測条件として、WH(Rot)(k=2)、LA(X)(k=3)、及びPB(Pitch)(k=13)を選択し、ランキングr=1での総和y^rを以下の(29)式により算出する。そして、ランキングr=1において、yとy^rとの誤差を表す指標Erを(28)式により算出する。 In the example of FIG. 8, the absolute value of the degree of contribution c k1 of the measurement condition (k = 3 to K) corresponding to the factor f = 1, and the contribution of the measurement condition (k = 3 to K) corresponding to the factor f = 3 As for the absolute value of the degree c k3 , the measurement condition (k = 3 to K) corresponding to the factor f = 5 is the largest in rotational angular acceleration PB (Pitch) (k = 13) about the y-direction center axis of the powertrain block 12 The absolute value of the degree of contribution c k5 ) is the largest in the x-direction translational acceleration LA (X) (k = 3) at the center of gravity of the unsprung element 15 (lower arm 19). Therefore, in the ranking r = 1, WH (Rot) (k = 2), LA (X) (k = 3), and PB (Pitch) (k = 13) are selected as a part of measurement conditions, and the ranking is The total sum ^ r at r = 1 is calculated by the following equation (29). Then, at ranking r = 1, an index E r representing an error between y and ^ r is calculated by equation (28).

y^r=d2×vec(X2)T+d3×vec(X3)T+d13×vec(X13)T (29) y ^ r = d 2 x vec (X 2 ) T + d 3 x vec (X 3 ) T + d 13 x vec (X 13 ) T (29)

因子f=1に対応する計測条件(k=3〜K)の寄与度ck1の絶対値は、パワートレインブロック12の重心点でのx方向並進加速度PB(X)(k=9)が2番目に大きく、因子f=3に対応する計測条件(k=3〜K)の寄与度ck3の絶対値は、ばね下要素15(ロワアーム19)の重心点でのz方向並進加速度LA(Z)(k=5)が2番目に大きく、因子f=5に対応する計測条件(k=3〜K)の寄与度ck5の絶対値は、パワートレインブロック12のz方向重心軸まわりの回転角加速度PB(Yaw)(k=14)が2番目に大きい。そこで、ランキングr=2では、一部の計測条件として、WH(Rot)(k=2)、LA(X)(k=3)、LA(Z)(k=5)、PB(X)(k=9)、PB(Pitch)(k=13)、及びPB(Yaw)(k=14)を選択し、ランキングr=2での総和y^rを以下の(30)式により算出する。そして、ランキングr=2において、yとy^rとの誤差を表す指標Erを(28)式により算出する。 The absolute value of the degree of contribution c k1 of the measurement condition (k = 3 to K) corresponding to the factor f = 1 is 2 in the x direction translational acceleration PB (X) (k = 9) at the center of gravity of the powertrain block 12 The absolute value of the contribution degree c k3 of the measurement condition (k = 3 to K) corresponding to the factor f = 3 is the z direction translational acceleration LA (Z (Z)) at the center of gravity of the unsprung element 15 (lower arm 19) The absolute value of the degree of contribution c k5 of the measurement condition (k = 3 to K) corresponding to the factor f = 5, where (k = 5) is the second largest, is the rotation of the powertrain block 12 about the center of gravity in the z direction. The angular acceleration PB (Yaw) (k = 14) is the second largest. Therefore, in the ranking r = 2, WH (Rot) (k = 2), LA (X) (k = 3), LA (Z) (k = 5), PB (X) (K = 5) as a part of measurement conditions. k = 9), PB (Pitch) (k = 13), and PB (Yaw) (k = 14) are selected, and the total sum ^ r at ranking r = 2 is calculated by the following equation (30). Then, at ranking r = 2, an index E r representing an error between y and ^ r is calculated by equation (28).

y^r=d2×vec(X2)T+d3×vec(X3)T+d5×vec(X5)T
+d9×vec(X9)T+d13×vec(X13)T+d14×vec(X14)T (30)
y ^ r = d 2 x vec (X 2 ) T + d 3 x vec (X 3 ) T + d 5 x vec (X 5 ) T
+ D 9 × vec (X 9 ) T + d 13 × vec (X 13 ) T + d 14 × vec (X 14 ) T (30)

因子f=1に対応する計測条件(k=3〜K)の寄与度ck1の絶対値は、パワートレインブロック12の重心点でのz方向並進加速度PB(Z)(k=11)が3番目に大きく、因子f=3に対応する計測条件(k=3〜K)の寄与度ck3の絶対値は、パワートレインブロック12のz方向重心軸まわりの回転角加速度PB(Yaw)(k=14)が3番目に大きく、因子f=5に対応する計測条件(k=3〜K)の寄与度ck5の絶対値は、ばね下要素15(ロワアーム19)のz方向重心軸まわりの回転角加速度LA(Yaw)(k=8)が3番目に大きい。そこで、ランキングr=3では、一部の計測条件として、WH(Rot)(k=2)、LA(X)(k=3)、LA(Z)(k=5)、LA(Yaw)(k=8)、PB(X)(k=9)、PB(Z)(k=11)、PB(Pitch)(k=13)、及びPB(Yaw)(k=14)を選択し、ランキングr=3での総和y^rを以下の(31)式により算出する。そして、ランキングr=3において、yとy^rとの誤差を表す指標Erを(28)式により算出する。さらに、同様の処理を繰り返すことで、ランキングr≧4において、yとy^rとの誤差を表す指標Erを(28)式により算出する。 The absolute value of the degree of contribution c k1 of the measurement condition (k = 3 to K) corresponding to the factor f = 1 is 3 in the z direction translational acceleration PB (Z) (k = 11) at the center of gravity of the powertrain block 12 The absolute value of the degree of contribution c k3 of the measurement condition (k = 3 to K) corresponding to the factor f = 3 is the rotational angular acceleration PB (Yaw) (k of the powertrain block 12 about the z axis) = 14) is the third largest, and the absolute value of the degree of contribution c k5 of the measurement condition (k = 3 to K) corresponding to the factor f = 5 is the z axis of gravity of the unsprung element 15 (lower arm 19) The rotational angular acceleration LA (Yaw) (k = 8) is the third largest. Therefore, in the ranking r = 3, WH (Rot) (k = 2), LA (X) (k = 3), LA (Z) (k = 5), LA (Yaw) (LAw) as a part of measurement conditions. Select k = 8), PB (X) (k = 9), PB (Z) (k = 11), PB (Pitch) (k = 13), and PB (Yaw) (k = 14), and rank them The total sum ^ r at r = 3 is calculated by the following equation (31). Then, at ranking r = 3, an index E r representing an error between y and y r is calculated by equation (28). Furthermore, by repeating the same process, in ranking r 表 す 4, an index E r representing an error between y and y r is calculated by equation (28).

y^r=d2×vec(X2)T+d3×vec(X3)T+d5×vec(X5)T
+d8×vec(X8)T+d9×vec(X9)T+d11×vec(X11)T
+d13×vec(X13)T+d14×vec(X14)T (31)
y ^ r = d 2 x vec (X 2 ) T + d 3 x vec (X 3 ) T + d 5 x vec (X 5 ) T
+ D 8 × vec (X 8 ) T + d 9 × vec (X 9 ) T + d 11 × vec (X 11 ) T
+ D 13 × vec (X 13 ) T + d 14 × vec (X 14 ) T (31)

ランキングrに対する指標Erの関係を計算した結果の一例を図9に示す。ただし、図9の縦軸の指標Erは、以下の(32)式で正規化している。図9には、振動解析モデルで考慮する計測条件(車体11のフロアのx方向並進加速度VE(X)及び駆動輪18の回転角加速度WH(Rot)を含む)の総数も示している。 An example of the result of calculating the relationship between the index E r and the ranking r is shown in FIG. However, the index E r on the vertical axis in FIG. 9 is normalized by the following equation (32). FIG. 9 also shows the total number of measurement conditions (including the x-direction translational acceleration VE (X) of the floor of the vehicle body 11 and the rotational angular acceleration WH (Rot) of the drive wheel 18) considered in the vibration analysis model.

図9の例では、ランキングr=2での指標Erが、ランキングr=1での指標Erに比べて大幅に減少している。一方、ランキングr≧3での指標Erは、ランキングr=2での指標Erとほとんど差がない。そこで、解析モデル同定部76は、車両10の振動解析モデルで考慮する計測条件を、指標Erが急速に減少する直後のランキングr=2で選択された計測条件である駆動輪18の回転振動、ばね下要素15(ロワアーム19)の重心点でのx方向並進振動とz方向並進振動、及びパワートレインブロック12の重心点でのx方向並進振動とy方向重心軸まわりの回転振動とz方向重心軸まわりの回転振動と、振動評価対象である車体11のフロアのx方向並進振動とに限定する。そして、解析モデル同定部76は、この限定した計測条件に基づいて車両10の振動解析モデルの構造同定を行う。なお、解析モデル同定部76は、車両10の振動解析モデルで考慮する計測条件を、振動評価対象である車体11のフロアのx方向並進振動と、指標Erが設定値以下となる最小のランキングrで選択された計測条件に限定することも可能である。 In the example of FIG. 9, the index E r at the ranking r = 2 is significantly reduced compared to the index E r at the ranking r = 1. On the other hand, the index E r of ranking r ≧ 3 has little difference indicative E r of the ranking r = 2. Therefore, the analysis model identification unit 76 determines the measurement condition to be considered in the vibration analysis model of the vehicle 10, the rotational vibration of the drive wheel 18, which is the measurement condition selected by the ranking r = 2 immediately after the index Er rapidly decreases. , X-direction translational vibration and z-direction translational vibration at the center of gravity of the unsprung element 15 (lower arm 19), x-direction translational vibration at the center of gravity of the powertrain block 12 and rotational vibration around the center of gravity y-axis It is limited to rotational vibration around the center of gravity axis and x-direction translational vibration of the floor of the vehicle body 11 that is the object of vibration evaluation. And the analysis model identification part 76 performs structure identification of the vibration analysis model of the vehicle 10 based on this limited measurement condition. The analysis model identification unit 76 determines the measurement conditions considered in the vibration analysis model of the vehicle 10, the x-direction translational vibration of the floor of the vehicle body 11 that is the vibration evaluation target, and the minimum ranking where the index E r is less than the set value. It is also possible to limit to the measurement conditions selected by r.

解析モデル同定部76で構造同定された車両10の振動解析モデルの一例を図10及び以下の(33)〜(41)式に示す。(33)〜(41)式については、以下の(42)式のように書き換えることができる。ただし、(33)〜(42)式では、時間微分を・(ドット)で表し、エンジン13の角加速度をθeの上に・・を付して表し、変速機14の角加速度をθmの上に・・を付して表し、駆動輪18の角加速度をθwの上に・・を付して表し、車体11のx方向並進加速度をxvの上に・・を付して表し、ばね下要素15のx方向並進加速度及びz方向並進加速度をxLA,zLAの上に・・を付して表し、パワートレインブロック12のx方向並進加速度、y方向重心軸まわりの角加速度、及びz方向重心軸まわりの角加速度をxPB,βPB,γPBの上に・・を付して表している。また、(33)〜(42)式において、Jeはエンジン13の慣性モーメント、Jmは変速機14の慣性モーメント、Jwは駆動輪18の慣性モーメント、mvは車体11の質量、mLAはばね下要素15の質量、mPBはパワートレインブロック12の質量、JβPBはパワートレインブロック12のy方向重心軸まわりの慣性モーメント、JγPBはパワートレインブロック12のz方向重心軸まわりの慣性モーメントである。τeはエンジン13のトルク(振動系の加振力)、τmはエンジン13と変速機14間で伝達されるトルク、dmは変速機14の変速比、τdsは変速機14と駆動輪18間で伝達されるトルク、Fdは駆動輪18と路面間に作用するx方向並進力、rwは駆動輪18の半径、Fx SSはばね下要素15と車体11間で伝達されるx方向並進力、Fx PBはパワートレインブロック12と車体11間で伝達されるx方向並進力、Fz SSはばね下要素15に作用するz方向並進力、τβPBはパワートレインブロック12に作用するy方向重心軸まわりのトルク、τγPBはパワートレインブロック12に作用するz方向重心軸まわりのトルクである。 An example of the vibration analysis model of the vehicle 10 structurally identified by the analysis model identification unit 76 is shown in FIG. 10 and the following equations (33) to (41). The equations (33) to (41) can be rewritten as the following equation (42). However, (33) in the - (42) below, represents the time derivative in. (Dot) represents the angular acceleration of the engine 13 are given the ... on the theta e, the angular acceleration of the transmission 14 theta m represents subjected to ... over the angular acceleration of the driving wheel 18 stands subjected to ... on the theta w, a x-direction translational acceleration of the vehicle body 11 denoted by the · on the x v Representing the x-direction translational acceleration of the unsprung element 15 and the z-direction translational acceleration by appending x LA , z LA on the x-direction translational acceleration of the powertrain block 12, an angle around the y-direction center of gravity axis The acceleration and the angular acceleration around the center of gravity axis in the z direction are indicated by adding ··· onto x PB , β PB , γ PB . Further, (33) to (42) below, J e is the moment of inertia of the engine 13, J m moment of inertia of the transmission 14, J w is the moment of inertia of the drive wheels 18, m v is the mass of the vehicle body 11, m LA is the mass of unsprung elements 15, m PB is the mass of the powertrain block 12, Jβ PB is the moment of inertia about the y-direction central axis of the power train block 12, Jγ PB is around the z-direction central axis of the power train block 12 It is a moment of inertia. τ e is the torque of the engine 13 (excitation force of the vibration system), τ m is the torque transmitted between the engine 13 and the transmission 14, d m is the transmission gear ratio of the transmission 14, and τ ds is the drive with the transmission 14 The torque transmitted between the wheels 18, F d is an x-direction translational force acting between the drive wheels 18 and the road surface, r w is the radius of the drive wheels 18, F x SS is transmitted between the unsprung element 15 and the vehicle body 11 that the x-direction translational force, F x PB is x-direction translation force transmitted between the powertrain block 12 and the vehicle body 11, F z SS is the z-direction translational force acting on the unsprung element 15, τβ PB powertrain block 12 Is a torque about the center of gravity y axis in the y direction, .tau..gamma. PB is a torque about the center of gravity z axis in the z direction acting on the power train block 12. As shown in FIG.

(33)〜(41)式((42)式)による振動解析モデルは、図10に示すような、複数の振動要素間の接続関係を表した原理モデルである。(33)式はエンジン13の回転運動方程式を表し、(34)式は変速機14の回転運動方程式を表し、(35)式は駆動輪18の回転運動方程式を表し、(36)式は車体11のx方向並進運動方程式を表し、(37)、(38)式はばね下要素15のx方向並進運動方程式及びz方向並進運動方程式を表し、(39)、(40)、(41)式はパワートレインブロック12のx方向並進運動方程式、y方向重心軸まわりの回転運動方程式、及びz方向重心軸まわりの回転運動方程式を表す。ただし、振動解析モデル(原理モデル)では、ばね下要素15の重心点でのy方向並進振動とx方向重心軸まわりの回転振動とy方向重心軸まわりの回転振動とz方向重心軸まわりの回転振動、及びパワートレインブロック12の重心点でのy方向並進振動とz方向並進振動とx方向重心軸まわりの回転振動については考慮されていない。つまり、車体11のx方向並進振動、エンジン13と変速機14と駆動輪18の回転振動、ばね下要素15の重心点でのx方向並進振動とz方向並進振動、及びパワートレインブロック12の重心点でのx方向並進振動とy方向重心軸まわりの回転振動とz方向重心軸まわりの回転振動だけを考慮した振動解析モデルに限定されている。   The vibration analysis model according to the equations (33) to (41) (equation (42)) is a principle model representing a connection relationship between a plurality of vibration elements as shown in FIG. (33) represents the rotational motion equation of the engine 13, (34) represents the rotational motion equation of the transmission 14, (35) represents the rotational motion equation of the drive wheel 18, and (36) represents the vehicle body Equations (37) and (38) represent the x-direction translational motion equation and the z-direction translational motion equation of the unsprung element 15, and the equations (39), (40) and (41) These represent the x-direction translational motion equation of the powertrain block 12, the rotational motion equation about the y-axis, and the rotational motion equation about the z-axis. However, in the vibration analysis model (principle model), the y-direction translational vibration at the center of gravity of the unsprung element 15, the rotational vibration around the x-axis, and the rotational vibration around the y-axis, and the rotation around the z-axis The vibration and the y-direction translational vibration at the center of gravity of the powertrain block 12, the z-direction translational vibration and the rotational vibration around the x-axis center of gravity are not taken into consideration. That is, the x-direction translational vibration of the vehicle body 11, the rotational vibrations of the engine 13, the transmission 14, and the drive wheel 18, the x-direction translational vibration and the z-direction translational vibration at the center of gravity of the unsprung element 15, and the center of gravity of the powertrain block 12 It is limited to a vibration analysis model that takes into account only the x-direction translational vibration at the point, the rotational vibration around the y-direction center of gravity axis, and the rotational vibration around the z-direction center of gravity axis.

振動解析装置70では、例えばエンジン13の角加速度、変速機14の角加速度、駆動輪18の角加速度、車体11のx方向並進加速度、ばね下要素15のx方向並進加速度とz方向並進加速度、及びパワートレインブロック12のx方向並進加速度とy方向重心軸まわりの角加速度とz方向重心軸まわりの角加速度を観測変数として取得することで、(33)〜(41)式((42)式)を用いて、未知変数である振動系の加振力τe、及び加振力τeにより各振動要素を伝わる伝達力τm,τds,Fd,Fx SS,Fz SS,Fx PB,τβPB,τγPBを推定することができる。そして、エンジン13のトルク(振動系の加振力)を入力、車体11のx方向並進加速度を出力とする場合における入出力の関係を表す伝達関数を算出することができる。また、振動要素を伝わる伝達力に基づいて振動要素間の弾性係数及び減衰係数を推定することもできる。 In the vibration analysis device 70, for example, the angular acceleration of the engine 13, the angular acceleration of the transmission 14, the angular acceleration of the drive wheel 18, the x direction translational acceleration of the vehicle body 11, the x direction translational acceleration of the unsprung element 15 and the z direction translational acceleration, And the angular acceleration around the x-direction translational acceleration of the powertrain block 12 and the y-direction center of gravity axis and the angular acceleration around the z-direction center of gravity axis as observation variables, the equations (33) to (41) (42) Transfer force τ m , τ ds , F d , F x SS , F z SS , F that propagates each vibration element by the vibration force τ e of the vibration system, which is unknown variable, and the vibration force τ e . It is possible to estimate x PB , τβ PB , τγ PB . Then, it is possible to calculate a transfer function representing the relationship between input and output when the torque of the engine 13 (the excitation force of the vibration system) is input and the x-direction translational acceleration of the vehicle body 11 is output. It is also possible to estimate the elastic coefficient and damping coefficient between the vibrating elements based on the transfer force transmitted through the vibrating elements.

以上説明した本実施形態では、振動計測対象とする振動要素及び振動計測方向のいずれか1つ以上が互いに異なる複数の計測条件での時系列振動データを取得する処理と、各時系列振動データをウェーブレット変換により時間及び周波数に対する振動データX1〜XKに変換する処理と、各振動データX1〜XKに対してPARAFAC解析を行うことで寄与度Cを算出する処理と、振動評価対象とする振動データX1とそれ以外の振動データX2〜XKと寄与度Cとの関係を表す(24)式に基づいて振動評価対象以外の各計測条件に対応する重み係数d2〜dKを算出する処理と、yとy^rとの誤差を表す指標Erに基づいて限定した計測条件により振動解析モデルの構造同定を行う処理とをコンピュータに実行させる。振動解析モデルの構造同定を行う処理においては、振動解析モデルで考慮する計測条件を、因子(f)に対応する寄与度c1f〜cKfがランキング上位にある必要最小限の計測条件に限定することができ、振動解析モデルを低次元化することができる。さらに、本実施形態における振動解析モデルの構造同定方法は、振動解析モデルを統計的に回帰する同定方法ではなく、平衡化打ち切り法等によって複雑な物理モデルから簡易モデルを導出する同定方法でもなく、構造同定された振動解析モデル(原理モデル)は物理的な意味を有する。したがって、振動解析モデルを低次元化しつつ精度を向上させることができる。なお、振動解析モデルの構造同定の際には、車両10の実稼働(実走行)時の振動データのみから実施可能であり、車両10よりパーツを降ろした単体計測は不要である。また、他の車両10との比較も容易であり、他の車両10がどのような思想で設計しているかを容易に把握することができる。 In the embodiment described above, processing for acquiring time-series vibration data under a plurality of measurement conditions in which any one or more of the vibration element to be subjected to vibration measurement and the vibration measurement direction are different from each other A process of converting the vibration data X 1 to X K with respect to time and frequency by wavelet transformation; a process of calculating a contribution degree C by performing PARAFAC analysis on each of the vibration data X 1 to X K ; Based on Eq. (24) representing the relationship between the vibration data X 1 and the other vibration data X 2 to X K and the degree of contribution C. The weighting coefficients d 2 to d K corresponding to the measurement conditions other than the vibration evaluation target And a process of identifying the structure of the vibration analysis model under a measurement condition limited based on the index E r representing the error between y and ^ r . In the process of structural identification of the vibration analysis model, the measurement conditions to be considered in the vibration analysis model are limited to the minimum necessary measurement conditions in which the contribution degrees c 1f to c Kf corresponding to the factor (f) are in the upper rankings The vibration analysis model can be reduced in dimension. Furthermore, the structure identification method of the vibration analysis model in the present embodiment is not an identification method that statistically regresses the vibration analysis model, but is not an identification method that derives a simplified model from a complex physical model by a balanced termination method or the like. The structurally identified vibration analysis model (principle model) has physical meaning. Therefore, the accuracy can be improved while reducing the dimension of the vibration analysis model. In addition, in the case of structure identification of a vibration analysis model, it can carry out only from the vibration data at the time of real operation (actual run) of vehicle 10, and the simple measurement which dropped parts from vehicle 10 is unnecessary. Moreover, comparison with other vehicles 10 is also easy, and it can be easily grasped what kind of idea the other vehicles 10 are designed.

さらに、本実施形態において、PARAFAC解析を行う処理では、各因子(f=1〜F)毎に算出した振動データ(aif×bjf)に基づいて因子(f)を選択することで、評価したい因子(f)に対応する振動モードを抽出することができ、抽出した振動モードを評価するための振動解析モデルの構造同定を行うことができる。さらに、aif×bjfの振幅の変動度合いが大きい過渡振動となる因子f=1,3,5を選択することで、評価したい因子f=1,3,5に対応する過渡振動を抽出することができ、過渡振動を評価するための振動解析モデルの構造同定を行うことができる。 Furthermore, in this embodiment, in the process of performing PARAFAC analysis, evaluation is performed by selecting the factor (f) based on the vibration data (a if x b jf ) calculated for each factor (f = 1 to F). A vibration mode corresponding to a desired factor (f) can be extracted, and structural identification of a vibration analysis model for evaluating the extracted vibration mode can be performed. Furthermore, by selecting the factor f = 1, 3, 5 in which the degree of fluctuation of the amplitude of a if × b jf is large, the transient vibration corresponding to the factor f = 1, 3, 5 to be evaluated is extracted It is possible to perform structural identification of a vibration analysis model for evaluating transient vibration.

以上の実施形態では、振動系が車両10である例について説明したが、本実施形態は車両以外の振動系に対しても適用可能である。   Although the above embodiment demonstrated the example whose vibration system was the vehicle 10, this embodiment is applicable also to vibration systems other than a vehicle.

以上、本発明を実施するための形態について説明したが、本発明はこうした実施形態に何等限定されるものではなく、本発明の要旨を逸脱しない範囲内において、種々なる形態で実施し得ることは勿論である。   As mentioned above, although the form for implementing this invention was demonstrated, this invention is not limited at all by such embodiment, It can be implemented with various forms in the range which does not deviate from the summary of this invention. Of course.

10 車両、11 車体、12 パワートレインブロック、13 エンジン、14 変速機、15 ばね下要素、16 マウント、17 サスペンションブッシュ、18 駆動輪、19 ロワアーム、21 加速度センサ、22−1,22−2,22−3,25−1,25−2,25−3 3軸加速度センサ、28 角速度センサ、70 振動解析装置、71 時系列振動データ取得部、72 設定定数記憶装置、73 振動データ変換部、74 因子解析部、75 重み係数算出部、76 解析モデル同定部。   Reference Signs List 10 vehicle, 11 vehicle body, 12 power train block, 13 engine, 14 transmission, 15 unsprung element, 16 mount, 17 suspension bush, 18 drive wheel, 19 lower arm, 21 acceleration sensor, 22-1, 22-2, 22 -3, 25-1, 25-2, 25-3 3-axis acceleration sensor, 28 angular velocity sensor, 70 vibration analysis device, 71 time series vibration data acquisition unit, 72 setting constant storage device, 73 vibration data conversion unit, 74 factor Analysis unit, 75 weight coefficient calculation unit, 76 analysis model identification unit.

Claims (2)

複数の振動要素を有する振動系の解析モデルの構造同定を行う振動解析モデルの構造同定装置であって、
振動系における振動計測対象とする振動要素及び振動計測方向のいずれか1つ以上が互いに異なる複数の計測条件での時系列振動データを取得する時系列振動データ取得部と、
時系列振動データ取得部で取得された各時系列振動データを、時間及び周波数に対する振動データに変換する振動データ変換部と、
振動データ変換部で変換された各振動データに対して因子数を変更して因子解析を行い、各因子数に対する因子解析の結果における振動データの変動度合いに応じて因子を選択し、当該因子に対応する各計測条件の寄与度を算出する因子解析部と、
振動データ変換部で変換された複数の計測条件での振動データにおいて、振動評価対象とする計測条件において計測された振動データと、それ以外の振動データと、因子解析部で算出された寄与度との関係に基づいて、振動評価対象以外の各計測条件に対応する重み係数を算出する重み係数算出部と、
振動データ変換部で変換された複数の計測条件での振動データにおいて、振動評価対象を除くすべての計測条件について重み係数で重み付けした振動データを加算した総和と、振動評価対象を除く因子解析部で算出された寄与度に基づいて選択された一部の計測条件について重み係数で重み付けした振動データを加算した総和との誤差を表す指標に基づいて計測条件を限定し、該限定した計測条件及び振動評価対象の計測条件に基づいて解析モデルの構造同定を行う解析モデル同定部と、
を備える、振動解析モデルの構造同定装置。
A structural identification device of a vibration analysis model for identifying the structure of an analysis model of a vibration system having a plurality of vibration elements,
A time-series vibration data acquisition unit that acquires time-series vibration data under a plurality of measurement conditions in which one or more of a vibration element to be subjected to vibration measurement and a vibration measurement direction in a vibration system are different from each other;
A vibration data conversion unit that converts each time-series vibration data acquired by the time-series vibration data acquisition unit into vibration data with respect to time and frequency;
There rows by changing the number of factors Factor analysis on the vibration data converted by the vibration data conversion unit selects a factor depending on the variation degree of the vibration data in the result of the factor analysis for each number of factors, the factors A factor analysis unit that calculates the degree of contribution of each measurement condition corresponding to
In the vibration data under a plurality of measurement conditions converted by the vibration data conversion unit, the vibration data measured under the measurement conditions targeted for vibration evaluation, the other vibration data, and the contribution degree calculated by the factor analysis unit A weighting factor calculation unit that calculates weighting factors corresponding to measurement conditions other than the vibration evaluation target based on the relationship of
In the vibration data under a plurality of measurement conditions converted by the vibration data conversion unit, the sum of the sum of the vibration data weighted by the weighting factor for all measurement conditions excluding the vibration evaluation target and the factor analysis unit excluding the vibration evaluation target The measurement conditions are limited based on an index that represents an error from the sum of the sum of the vibration data weighted by the weighting factor for a part of the measurement conditions selected based on the calculated degree of contribution , and the limited measurement conditions and the vibration An analysis model identification unit that identifies the structure of the analysis model based on the measurement conditions to be evaluated ;
A structural identification device of a vibration analysis model, comprising:
複数の振動要素を有する振動系の解析モデルの構造同定を行う振動解析モデルの構造同定方法であって、
振動系における振動計測対象とする振動要素及び振動計測方向のいずれか1つ以上が互いに異なる複数の計測条件での時系列振動データを取得する時系列振動データ取得処理と、
時系列振動データ取得処理で取得された各時系列振動データを、時間及び周波数に対する振動データに変換する振動データ変換処理と、
振動データ変換処理で変換された各振動データに対して因子数を変更して因子解析を行い、各因子数に対する因子解析の結果における振動データの変動度合いに応じて因子を選択し、当該因子に対応する各計測条件の寄与度を算出する因子解析処理と、
振動データ変換処理で変換された複数の計測条件での振動データにおいて、振動評価対象とする計測条件において計測された振動データと、それ以外の振動データと、因子解析処理で算出された寄与度との関係に基づいて、振動評価対象以外の各計測条件に対応する重み係数を算出する重み係数算出処理と、
振動データ変換処理で変換された複数の計測条件での振動データにおいて、振動評価対象を除くすべての計測条件について重み係数で重み付けした振動データを加算した総和と、振動評価対象を除く因子解析部で算出された寄与度に基づいて選択された一部の計測条件について重み係数で重み付けした振動データを加算した総和との誤差を表す指標に基づいて計測条件を限定し、該限定した計測条件及び振動評価対象の計測条件に基づいて解析モデルの構造同定を行う解析モデル同定処理と、
を含む、振動解析モデルの構造同定方法。
A structure identification method of a vibration analysis model for identifying a structure of an analysis model of a vibration system having a plurality of vibration elements,
Time-series vibration data acquisition processing for acquiring time-series vibration data under a plurality of measurement conditions in which any one or more of a vibration element to be subjected to vibration measurement and a vibration measurement direction in a vibration system are different from each other;
Vibration data conversion processing for converting each time-series vibration data acquired in the time-series vibration data acquisition processing into vibration data with respect to time and frequency;
There rows by changing the number of factors Factor analysis on the vibration data converted by the vibration data conversion process, and select the factor in accordance with the fluctuation degree of the vibration data in the result of the factor analysis for each number of factors, the factors Factor analysis processing to calculate the degree of contribution of each measurement condition corresponding to
In the vibration data under a plurality of measurement conditions converted by the vibration data conversion process, the vibration data measured under the measurement conditions to be evaluated for vibration, the other vibration data, and the contribution degree calculated by the factor analysis process Weight coefficient calculation processing for calculating a weight coefficient corresponding to each measurement condition other than the vibration evaluation target based on the relationship of
In the vibration data under multiple measurement conditions converted by the vibration data conversion process, the sum of the sum of the vibration data weighted by the weighting factor for all measurement conditions excluding the vibration evaluation target, and the factor analysis unit excluding the vibration evaluation target The measurement conditions are limited based on an index that represents an error from the sum of the sum of the vibration data weighted by the weighting factor for a part of the measurement conditions selected based on the calculated degree of contribution , and the limited measurement conditions and the vibration Analysis model identification processing for identifying the structure of the analysis model based on the measurement condition to be evaluated ;
How to identify the structure of vibration analysis model, including
JP2015097479A 2015-05-12 2015-05-12 Structure identification device for vibration analysis model and identification method thereof Active JP6535208B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2015097479A JP6535208B2 (en) 2015-05-12 2015-05-12 Structure identification device for vibration analysis model and identification method thereof

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2015097479A JP6535208B2 (en) 2015-05-12 2015-05-12 Structure identification device for vibration analysis model and identification method thereof

Publications (2)

Publication Number Publication Date
JP2016212016A JP2016212016A (en) 2016-12-15
JP6535208B2 true JP6535208B2 (en) 2019-06-26

Family

ID=57551054

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2015097479A Active JP6535208B2 (en) 2015-05-12 2015-05-12 Structure identification device for vibration analysis model and identification method thereof

Country Status (1)

Country Link
JP (1) JP6535208B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP7074113B2 (en) * 2019-09-02 2022-05-24 株式会社豊田中央研究所 Vehicle characteristic optimization device, vehicle characteristic optimization method and program
CN114184192B (en) * 2021-12-27 2023-09-26 北京计算机技术及应用研究所 Method for acquiring angular velocity measurement channel transfer function of inertial measurement device

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010048684A (en) * 2008-08-22 2010-03-04 Univ Of Tokyo Vibration analyzer and vibration analysis method

Also Published As

Publication number Publication date
JP2016212016A (en) 2016-12-15

Similar Documents

Publication Publication Date Title
Law et al. Moving force identification: optimal state estimation approach
Law et al. Vehicle axle loads identification using finite element method
Zhu et al. Moving forces identification on a multi-span continuous bridge
JP6090336B2 (en) Vehicle vibration analysis method and vibration analysis apparatus
Dodds et al. Laboratory road simulation for full vehicle testing: a review
JP6848813B2 (en) Information processing equipment, information processing methods and programs
CN103003680A (en) Rigid body characteristic recognition device and rigid body characteristic recognition method
Law et al. Study on different beam models in moving force identification
CN111079323A (en) Dynamic response prediction method and system based on human-vehicle-road coupled vibration model
JP6535208B2 (en) Structure identification device for vibration analysis model and identification method thereof
JP7024874B2 (en) Inspection system, inspection method, and program
Kilikevičienė et al. The analysis of bus air spring condition influence upon the vibration signals at bus frame
Kilikevičius et al. The analysis of vibration signals of critical points of the Bus Body Frame
Wang et al. Data-based deep learning for random vibration fatigue life prediction of car seat frame
Farroni et al. Experimental Methodology for Tire Ride Analysis Based on Outdoor Cleat Testing
Jang et al. A feasible strain-history extraction method using machine learning for the durability evaluation of automotive parts
CN114096454B (en) Estimation device, estimation method, and storage medium
Gurmai et al. A comparative study of destructive effects resulting from road profile acting on off-road towed vehicles
Zeitvogel et al. Holistic vehicle parametrization on a handling roadway
Žuraulis et al. Quarter car test rig for extended dynamics research in laboratory conditions
Uechi et al. The Profiling of International Roughness Index (IRI) Based on Lagrangian Method
JP6260477B2 (en) Vibration analysis apparatus and vibration analysis method
JP2003287461A (en) Vibration analytical method for object to be measured symmetric with respect to central axis, program for executing the same and computer-readable recording medium with recorded program
JP2019100745A (en) Oscillation analysis model structure identification device, and oscillation analysis model structure identification method
MAEDA et al. Coupling analysis of unsteady aerodynamics and vehicle behavior with road input: Modeling and verification in road tests

Legal Events

Date Code Title Description
A621 Written request for application examination

Free format text: JAPANESE INTERMEDIATE CODE: A621

Effective date: 20170810

A977 Report on retrieval

Free format text: JAPANESE INTERMEDIATE CODE: A971007

Effective date: 20180709

A131 Notification of reasons for refusal

Free format text: JAPANESE INTERMEDIATE CODE: A131

Effective date: 20180904

A521 Request for written amendment filed

Free format text: JAPANESE INTERMEDIATE CODE: A523

Effective date: 20181101

TRDD Decision of grant or rejection written
A01 Written decision to grant a patent or to grant a registration (utility model)

Free format text: JAPANESE INTERMEDIATE CODE: A01

Effective date: 20190521

A61 First payment of annual fees (during grant procedure)

Free format text: JAPANESE INTERMEDIATE CODE: A61

Effective date: 20190531

R150 Certificate of patent or registration of utility model

Ref document number: 6535208

Country of ref document: JP

Free format text: JAPANESE INTERMEDIATE CODE: R150

R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250

R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250

R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250

R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250