Fast detectionofsystemnonlinearityusingnonstationarysignals
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smart weldingintelli WELD ®Typical Applications:• Robot-assisted welding (“remote welding”) • 3D applications• Processing-on-the-flyDesigned for robot-assisted welding applications, this 3D-scan system is capable of swiftly positioning the laser beam along 3D contours. While a robot guides the scan system along a part’s contour, the intelli WELD ® quickly and accurately moves and fine-positions the laser spot. Complex robotic motions and fast robotic repositioning are thereby avoided, thus reducing positioning times between spot welds to a few milliseconds. The result is a substan-tially enhanced utilization of the laser source.Despite its 30 mm aperture, the intelli WELD ® occupies a remark-ably small volume, making it easily mountable on welding robots,even in difficult-to-access locations. Its optics are optimized for fiber-coupled disk or fiber lasers with powers up to 8 kW. The intelli WELD ® is based on SCANLAB’s fully digital i DRIVE ® technology, offering an integrated approach to laser and process safety. The technology allows real-time monitoring of all important scan head status parameters. A software-independent interlock signal indicates abnormal operational states.SCANLAB America, Inc. · 100 Illinois St · St. Charles, IL 60174 · USA Tel. +1 (630) 797-2044 · Fax +1 (630) 797-2001info@ · SCANLAB AG · Siemensstr. 2a · 82178 Puchheim · Germany Tel. +49 (89) 800 746-0 · Fax +49 (89) 800 746-199 info@scanlab.de · www.scanlab.de Specifications (all angles are in optical degrees) Wavelength1030 nm - 1085 nm (1)Maximum laser power(with specified cooling)8000 WCharacteristics of the collimator Focal length 110 mm Limiting numerical aperture typ. 0.125 (2)Fiber adapterQBH , Q 5 /L LK-B, Q D /L LK-D (other types on request)Step response time (with step tuning)(settling to 1/1000 of full scale)1% of full scale 1.2 ms 10% of full scale 3.5 ms 100% of full scale 11 ms Typical speeds (with vector tuning)Processing Speed 4 rad/s Positioning Speed 50 rad/s Dynamic performance Tracking error 0.6 ms Repeatability (RMS)< 2 µrad Long-term drift over 8 h (after warm-up)< 0.6 mradOptical performance Typical scan angle ±0.35 rad Gain error < 5 mradNonlinearity< 3.5 mrad / 44°Power requirements±(15+1.5) V DC, max. 8 A eachInput and output signals SL2-100 oroptical data transfer (XY2-100-O)Weight 21 - 37 kg Operating temperature 25 °C ± 10 °C Typical water requirements3 l/min at 20°C and∆p < 0.1 bar, p < 4 bar (1)mirror coatings for 1030 nm, 1055 - 1085 nm and1070 - 1085 nm are currently available (2)adapters for smaller numerical apertures are availableTypical Optical ConfigurationsPre-Objective scanningPost-Objective scanning Focal length of focusing optics 330 mm 460 mm660 mm Free operating distance 382 mm 488 mm472 mmImage volume size(cuboid-shaped)(185 x 185 x 80) mm 3(220 x 220 x 140) mm 3(370 x 370 x 200) mm 3Image field size (elliptical)(240 x 200) mm 2(385 x 270) mm 2approx. (450 x 450) mm 2Focus range in z direction ±40 mm ±70 mm up to ±100 mm Focus diameter 600 µm(with 200 µm fiber)630 µm(with 150 µm fiber)600 µm(with 100 µm fiber)Fiber diameter 150 µm or 200 µm 100 µm, 150 µm or 200 µm 50 µm or 100 µm Image scale1:31:41:612 / 2014 I n f o r m a t i o n i s s u b j e c t t o c h a n g e w i t h o u t n o t i c e . P r o d u c t p h o t o s a r e n o n -b i n d i n g a n d m a y s h o w c u s t o m i z e d f e a t u r e s .。
(完整版)自动控制专业英语词汇自动控制专业英语词汇(一)acceleration transducer 加速度传感器acceptance testing 验收测试accessibility 可及性accumulated error 累积误差AC-DC-AC frequency converter 交-直-交变频器AC (alternating current) electric drive 交流电子传动active attitude stabilization 主动姿态稳定actuator 驱动器,执行机构adaline 线性适应元adaptation layer 适应层adaptive telemeter system 适应遥测系统adjoint operator 伴随算子admissible error 容许误差aggregation matrix 集结矩阵AHP (analytic hierarchy process) 层次分析法amplifying element 放大环节analog-digital conversion 模数转换annunciator 信号器antenna pointing control 天线指向控制anti-integral windup 抗积分饱卷aperiodic decomposition 非周期分解a posteriori estimate 后验估计approximate reasoning 近似推理a priori estimate 先验估计articulated robot 关节型机器人assignment problem 配置问题,分配问题associative memory model 联想记忆模型associatron 联想机asymptotic stability 渐进稳定性attained pose drift 实际位姿漂移attitude acquisition 姿态捕获AOCS (attritude and orbit control system) 姿态轨道控制系统attitude angular velocity 姿态角速度attitude disturbance 姿态扰动attitude maneuver 姿态机动attractor 吸引子augment ability 可扩充性augmented system 增广系统automatic manual station 自动-手动操作器automaton 自动机autonomous system 自治系统backlash characteristics 间隙特性base coordinate system 基座坐标系Bayes classifier 贝叶斯分类器bearing alignment 方位对准bellows pressure gauge 波纹管压力表benefit-cost analysis 收益成本分析bilinear system 双线性系统biocybernetics 生物控制论biological feedback system 生物反馈系统black box testing approach 黑箱测试法blind search 盲目搜索block diagonalization 块对角化Boltzman machine 玻耳兹曼机bottom-up development 自下而上开发boundary value analysis 边界值分析brainstorming method 头脑风暴法breadth-first search 广度优先搜索butterfly valve 蝶阀CAE (computer aided engineering) 计算机辅助工程CAM (computer aided manufacturing) 计算机辅助制造Camflex valve 偏心旋转阀canonical state variable 规范化状态变量capacitive displacement transducer 电容式位移传感器capsule pressure gauge 膜盒压力表CARD 计算机辅助研究开发Cartesian robot 直角坐标型机器人cascade compensation 串联补偿catastrophe theory 突变论centrality 集中性chained aggregation 链式集结chaos 混沌characteristic locus 特征轨迹chemical propulsion 化学推进calrity 清晰性classical information pattern 经典信息模式classifier 分类器clinical control system 临床控制系统closed loop pole 闭环极点closed loop transfer function 闭环传递函数cluster analysis 聚类分析coarse-fine control 粗-精控制cobweb model 蛛网模型coefficient matrix 系数矩阵cognitive science 认知科学cognitron 认知机coherent system 单调关联系统combination decision 组合决策combinatorial explosion 组合爆炸combined pressure and vacuum gauge 压力真空表command pose 指令位姿companion matrix 相伴矩阵compartmental model 房室模型compatibility 相容性,兼容性compensating network 补偿网络compensation 补偿,矫正compliance 柔顺,顺应composite control 组合控制computable general equilibrium model 可计算一般均衡模型conditionally instability 条件不稳定性configuration 组态connectionism 连接机制connectivity 连接性conservative system 守恒系统consistency 一致性constraint condition 约束条件consumption function 消费函数context-free grammar 上下文无关语法continuous discrete event hybrid system simulation 连续离散事件混合系统仿真continuous duty 连续工作制control accuracy 控制精度control cabinet 控制柜controllability index 可控指数controllable canonical form 可控规范型[control] plant 控制对象,被控对象controlling instrument 控制仪表control moment gyro 控制力矩陀螺control panel 控制屏,控制盘control synchro 控制[式]自整角机control system synthesis 控制系统综合control time horizon 控制时程cooperative game 合作对策coordinability condition 可协调条件coordination strategy 协调策略coordinator 协调器corner frequency 转折频率costate variable 共态变量cost-effectiveness analysis 费用效益分析coupling of orbit and attitude 轨道和姿态耦合critical damping 临界阻尼critical stability 临界稳定性cross-over frequency 穿越频率,交越频率current source inverter 电流[源]型逆变器cut-off frequency 截止频率cybernetics 控制论cyclic remote control 循环遥控cylindrical robot 圆柱坐标型机器人damped oscillation 阻尼振荡damper 阻尼器damping ratio 阻尼比data acquisition 数据采集data encryption 数据加密data preprocessing 数据预处理data processor 数据处理器DC generator-motor set drive 直流发电机-电动机组传动D controller 微分控制器decentrality 分散性decentralized stochastic control 分散随机控制decision space 决策空间decision support system 决策支持系统decomposition-aggregation approach 分解集结法decoupling parameter 解耦参数deductive-inductive hybrid modeling method 演绎与归纳混合建模法delayed telemetry 延时遥测derivation tree 导出树derivative feedback 微分反馈describing function 描述函数desired value 希望值despinner 消旋体destination 目的站detector 检出器deterministic automaton 确定性自动机deviation 偏差deviation alarm 偏差报警器DFD 数据流图diagnostic model 诊断模型diagonally dominant matrix 对角主导矩阵diaphragm pressure gauge 膜片压力表difference equation model 差分方程模型differential dynamical system 微分动力学系统differential game 微分对策differential pressure level meter 差压液位计differential pressure transmitter 差压变送器differential transformer displacement transducer 差动变压器式位移传感器differentiation element 微分环节digital filer 数字滤波器digital signal processing 数字信号处理digitization 数字化digitizer 数字化仪dimension transducer 尺度传感器direct coordination 直接协调disaggregation 解裂discoordination 失协调discrete event dynamic system 离散事件动态系统discrete system simulation language 离散系统仿真语言discriminant function 判别函数displacement vibration amplitude transducer 位移振幅传感器dissipative structure 耗散结构distributed parameter control system 分布参数控制系统distrubance 扰动disturbance compensation 扰动补偿diversity 多样性divisibility 可分性domain knowledge 领域知识dominant pole 主导极点dose-response model 剂量反应模型dual modulation telemetering system 双重调制遥测系统dual principle 对偶原理dual spin stabilization 双自旋稳定duty ratio 负载比dynamic braking 能耗制动dynamic characteristics 动态特性dynamic deviation 动态偏差dynamic error coefficient 动态误差系数dynamic exactness 动它吻合性dynamic input-output model 动态投入产出模型econometric model 计量经济模型economic cybernetics 经济控制论economic effectiveness 经济效益economic evaluation 经济评价economic index 经济指数economic indicator 经济指标eddy current thickness meter 电涡流厚度计effectiveness 有效性effectiveness theory 效益理论elasticity of demand 需求弹性electric actuator 电动执行机构electric conductance levelmeter 电导液位计electric drive control gear 电动传动控制设备electric hydraulic converter 电-液转换器electric pneumatic converter 电-气转换器electrohydraulic servo vale 电液伺服阀electromagnetic flow transducer 电磁流量传感器electronic batching scale 电子配料秤electronic belt conveyor scale 电子皮带秤electronic hopper scale 电子料斗秤elevation 仰角emergency stop 异常停止empirical distribution 经验分布endogenous variable 内生变量equilibrium growth 均衡增长equilibrium point 平衡点equivalence partitioning 等价类划分ergonomics 工效学error 误差error-correction parsing 纠错剖析estimate 估计量estimation theory 估计理论evaluation technique 评价技术event chain 事件链evolutionary system 进化系统exogenous variable 外生变量expected characteristics 希望特性external disturbance 外扰fact base 事实failure diagnosis 故障诊断fast mode 快变模态feasibility study 可行性研究feasible coordination 可行协调feasible region 可行域feature detection 特征检测feature extraction 特征抽取feedback compensation 反馈补偿feedforward path 前馈通路field bus 现场总线finite automaton 有限自动机FIP (factory information protocol) 工厂信息协议first order predicate logic 一阶谓词逻辑fixed sequence manipulator 固定顺序机械手fixed set point control 定值控制FMS (flexible manufacturing system) 柔性制造系统flow sensor/transducer 流量传感器flow transmitter 流量变送器fluctuation 涨落forced oscillation 强迫振荡formal language theory 形式语言理论formal neuron 形式神经元forward path 正向通路forward reasoning 正向推理fractal 分形体,分维体frequency converter 变频器frequency domain model reduction method 频域模型降阶法frequency response 频域响应full order observer 全阶观测器functional decomposition 功能分解FES (functional electrical stimulation) 功能电刺激functional simularity 功能相似fuzzy logic 模糊逻辑game tree 对策树gate valve 闸阀general equilibrium theory 一般均衡理论generalized least squares estimation 广义最小二乘估计generation function 生成函数geomagnetic torque 地磁力矩geometric similarity 几何相似gimbaled wheel 框架轮global asymptotic stability 全局渐进稳定性global optimum 全局最优globe valve 球形阀goal coordination method 目标协调法grammatical inference 文法推断graphic search 图搜索gravity gradient torque 重力梯度力矩group technology 成组技术guidance system 制导系统gyro drift rate 陀螺漂移率gyrostat 陀螺体Hall displacement transducer 霍尔式位移传感器hardware-in-the-loop simulation 半实物仿真harmonious deviation 和谐偏差harmonious strategy 和谐策略heuristic inference 启发式推理hidden oscillation 隐蔽振荡hierarchical chart 层次结构图hierarchical planning 递阶规划hierarchical control 递阶控制homeostasis 内稳态homomorphic model 同态系统horizontal decomposition 横向分解hormonal control 内分泌控制hydraulic step motor 液压步进马达hypercycle theory 超循环理论I controller 积分控制器identifiability 可辨识性IDSS (intelligent decision support system) 智能决策支持系统image recognition 图像识别impulse 冲量impulse function 冲击函数,脉冲函数inching 点动incompatibility principle 不相容原理incremental motion control 增量运动控制index of merit 品质因数inductive force transducer 电感式位移传感器inductive modeling method 归纳建模法industrial automation 工业自动化inertial attitude sensor 惯性姿态敏感器inertial coordinate system 惯性坐标系inertial wheel 惯性轮inference engine 推理机infinite dimensional system 无穷维系统information acquisition 信息采集infrared gas analyzer 红外线气体分析器inherent nonlinearity 固有非线性inherent regulation 固有调节initial deviation 初始偏差initiator 发起站injection attitude 入轨姿势input-output model 投入产出模型instability 不稳定性instruction level language 指令级语言integral of absolute value of error criterion 绝对误差积分准则integral of squared error criterion 平方误差积分准则integral performance criterion 积分性能准则integration instrument 积算仪器integrity 整体性intelligent terminal 智能终端interacted system 互联系统,关联系统interactive prediction approach 互联预估法,关联预估法interconnection 互联intermittent duty 断续工作制internal disturbance 内扰ISM (interpretive structure modeling) 解释结构建模法invariant embedding principle 不变嵌入原理inventory theory 库伦论inverse Nyquist diagram 逆奈奎斯特图inverter 逆变器investment decision 投资决策isomorphic model 同构模型iterative coordination 迭代协调jet propulsion 喷气推进job-lot control 分批控制joint 关节Kalman-Bucy filer 卡尔曼-布西滤波器knowledge accomodation 知识顺应knowledge acquisition 知识获取knowledge assimilation 知识同化KBMS (knowledge base management system) 知识库管理系统knowledge representation 知识表达ladder diagram 梯形图lag-lead compensation 滞后超前补偿Lagrange duality 拉格朗日对偶性Laplace transform 拉普拉斯变换large scale system 大系统lateral inhibition network 侧抑制网络least cost input 最小成本投入least squares criterion 最小二乘准则level switch 物位开关libration damping 天平动阻尼limit cycle 极限环linearization technique 线性化方法linear motion electric drive 直线运动电气传动linear motion valve 直行程阀linear programming 线性规划LQR (linear quadratic regulator problem) 线性二次调节器问题load cell 称重传感器local asymptotic stability 局部渐近稳定性local optimum 局部最优log magnitude-phase diagram 对数幅相图long term memory 长期记忆lumped parameter model 集总参数模型Lyapunov theorem of asymptotic stability 李雅普诺夫渐近稳定性定理自动控制专业英语词汇(二)macro-economic system 宏观经济系统magnetic dumping 磁卸载magnetoelastic weighing cell 磁致弹性称重传感器magnitude-frequency characteristic 幅频特性magnitude margin 幅值裕度magnitude scale factor 幅值比例尺manipulator 机械手man-machine coordination 人机协调manual station 手动操作器MAP (manufacturing automation protocol) 制造自动化协议marginal effectiveness 边际效益Mason's gain formula 梅森增益公式master station 主站matching criterion 匹配准则maximum likelihood estimation 最大似然估计maximum overshoot 最大超调量maximum principle 极大值原理mean-square error criterion 均方误差准则mechanism model 机理模型meta-knowledge 元知识metallurgical automation 冶金自动化minimal realization 最小实现minimum phase system 最小相位系统minimum variance estimation 最小方差估计minor loop 副回路missile-target relative movement simulator 弹体-目标相对运动仿真器modal aggregation 模态集结modal transformation 模态变换MB (model base) 模型库model confidence 模型置信度model fidelity 模型逼真度model reference adaptive control system 模型参考适应控制系统model verification 模型验证modularization 模块化MEC (most economic control) 最经济控制motion space 可动空间MTBF (mean time between failures) 平均故障间隔时间MTTF (mean time to failures) 平均无故障时间multi-attributive utility function 多属性效用函数multicriteria 多重判据multilevel hierarchical structure 多级递阶结构multiloop control 多回路控制multi-objective decision 多目标决策multistate logic 多态逻辑multistratum hierarchical control 多段递阶控制multivariable control system 多变量控制系统myoelectric control 肌电控制Nash optimality 纳什最优性natural language generation 自然语言生成nearest-neighbor 最近邻necessity measure 必然性侧度negative feedback 负反馈neural assembly 神经集合neural network computer 神经网络计算机Nichols chart 尼科尔斯图noetic science 思维科学noncoherent system 非单调关联系统noncooperative game 非合作博弈nonequilibrium state 非平衡态nonlinear element 非线性环节nonmonotonic logic 非单调逻辑nonparametric training 非参数训练nonreversible electric drive 不可逆电气传动nonsingular perturbation 非奇异摄动non-stationary random process 非平稳随机过程nuclear radiation levelmeter 核辐射物位计nutation sensor 章动敏感器Nyquist stability criterion 奈奎斯特稳定判据objective function 目标函数observability index 可观测指数observable canonical form 可观测规范型on-line assistance 在线帮助on-off control 通断控制open loop pole 开环极点operational research model 运筹学模型optic fiber tachometer 光纤式转速表optimal trajectory 最优轨迹optimization technique 最优化技术orbital rendezvous 轨道交会orbit gyrocompass 轨道陀螺罗盘orbit perturbation 轨道摄动order parameter 序参数orientation control 定向控制originator 始发站oscillating period 振荡周期output prediction method 输出预估法oval wheel flowmeter 椭圆齿轮流量计overall design 总体设计overdamping 过阻尼overlapping decomposition 交叠分解Pade approximation 帕德近似Pareto optimality 帕雷托最优性passive attitude stabilization 被动姿态稳定path repeatability 路径可重复性pattern primitive 模式基元PR (pattern recognition) 模式识别P control 比例控制器peak time 峰值时间penalty function method 罚函数法perceptron 感知器periodic duty 周期工作制perturbation theory 摄动理论pessimistic value 悲观值phase locus 相轨迹phase trajectory 相轨迹phase lead 相位超前photoelectric tachometric transducer 光电式转速传感器phrase-structure grammar 短句结构文法physical symbol system 物理符号系统piezoelectric force transducer 压电式力传感器playback robot 示教再现式机器人PLC (programmable logic controller) 可编程序逻辑控制器plug braking 反接制动plug valve 旋塞阀pneumatic actuator 气动执行机构point-to-point control 点位控制polar robot 极坐标型机器人pole assignment 极点配置pole-zero cancellation 零极点相消polynomial input 多项式输入portfolio theory 投资搭配理论pose overshoot 位姿过调量position measuring instrument 位置测量仪posentiometric displacement transducer 电位器式位移传感器positive feedback 正反馈power system automation 电力系统自动化predicate logic 谓词逻辑pressure gauge with electric contact 电接点压力表pressure transmitter 压力变送器price coordination 价格协调primal coordination 主协调primary frequency zone 主频区PCA (principal component analysis) 主成分分析法principle of turnpike 大道原理priority 优先级process-oriented simulation 面向过程的仿真production budget 生产预算production rule 产生式规则profit forecast 利润预测PERT (program evaluation and review technique) 计划评审技术program set station 程序设定操作器proportional control 比例控制proportional plus derivative controller 比例微分控制器protocol engineering 协议工程prototype 原型pseudo random sequence 伪随机序列pseudo-rate-increment control 伪速率增量控制pulse duration 脉冲持续时间pulse frequency modulation control system 脉冲调频控制系统pulse width modulation control system 脉冲调宽控制系统PWM inverter 脉宽调制逆变器pushdown automaton 下推自动机QC (quality control) 质量管理quadratic performance index 二次型性能指标qualitative physical model 定性物理模型quantized noise 量化噪声quasilinear characteristics 准线性特性queuing theory 排队论radio frequency sensor 射频敏感器ramp function 斜坡函数random disturbance 随机扰动random process 随机过程rate integrating gyro 速率积分陀螺ratio station 比值操作器reachability 可达性reaction wheel control 反作用轮控制realizability 可实现性,能实现性real time telemetry 实时遥测receptive field 感受野rectangular robot 直角坐标型机器人rectifier 整流器recursive estimation 递推估计reduced order observer 降阶观测器redundant information 冗余信息reentry control 再入控制regenerative braking 回馈制动,再生制动regional planning model 区域规划模型regulating device 调节装载regulation 调节relational algebra 关系代数relay characteristic 继电器特性remote manipulator 遥控操作器remote regulating 遥调remote set point adjuster 远程设定点调整器rendezvous and docking 交会和对接reproducibility 再现性resistance thermometer sensor 热电阻resolution principle 归结原理resource allocation 资源分配response curve 响应曲线return difference matrix 回差矩阵return ratio matrix 回比矩阵reverberation 回响reversible electric drive 可逆电气传动revolute robot 关节型机器人revolution speed transducer 转速传感器rewriting rule 重写规则rigid spacecraft dynamics 刚性航天动力学risk decision 风险分析robotics 机器人学robot programming language 机器人编程语言robust control 鲁棒控制robustness 鲁棒性roll gap measuring instrument 辊缝测量仪root locus 根轨迹roots flowmeter 腰轮流量计rotameter 浮子流量计,转子流量计rotary eccentric plug valve 偏心旋转阀rotary motion valve 角行程阀rotating transformer 旋转变压器Routh approximation method 劳思近似判据routing problem 路径问题sampled-data control system 采样控制系统sampling control system 采样控制系统saturation characteristics 饱和特性scalar Lyapunov function 标量李雅普诺夫函数SCARA (selective compliance assembly robot arm) 平面关节型机器人scenario analysis method 情景分析法scene analysis 物景分析s-domain s域self-operated controller 自力式控制器self-organizing system 自组织系统self-reproducing system 自繁殖系统self-tuning control 自校正控制semantic network 语义网络semi-physical simulation 半实物仿真sensing element 敏感元件sensitivity analysis 灵敏度分析sensory control 感觉控制sequential decomposition 顺序分解sequential least squares estimation 序贯最小二乘估计servo control 伺服控制,随动控制servomotor 伺服马达settling time 过渡时间sextant 六分仪short term planning 短期计划short time horizon coordination 短时程协调signal detection and estimation 信号检测和估计signal reconstruction 信号重构similarity 相似性simulated interrupt 仿真中断simulation block diagram 仿真框图simulation experiment 仿真实验simulation velocity 仿真速度simulator 仿真器single axle table 单轴转台single degree of freedom gyro 单自由度陀螺single level process 单级过程single value nonlinearity 单值非线性singular attractor 奇异吸引子singular perturbation 奇异摄动sink 汇点slaved system 受役系统slower-than-real-time simulation 欠实时仿真slow subsystem 慢变子系统socio-cybernetics 社会控制论socioeconomic system 社会经济系统software psychology 软件心理学solar array pointing control 太阳帆板指向控制solenoid valve 电磁阀source 源点specific impulse 比冲speed control system 调速系统spin axis 自旋轴spinner 自旋体stability criterion 稳定性判据stability limit 稳定极限stabilization 镇定,稳定Stackelberg decision theory 施塔克尔贝格决策理论state equation model 状态方程模型state space description 状态空间描述static characteristics curve 静态特性曲线station accuracy 定点精度stationary random process 平稳随机过程statistical analysis 统计分析statistic pattern recognition 统计模式识别steady state deviation 稳态偏差steady state error coefficient 稳态误差系数step-by-step control 步进控制step function 阶跃函数stepwise refinement 逐步精化stochastic finite automaton 随机有限自动机strain gauge load cell 应变式称重传感器strategic function 策略函数strongly coupled system 强耦合系统subjective probability 主观频率suboptimality 次优性supervised training 监督学习supervisory computer control system 计算机监控系统sustained oscillation 自持振荡swirlmeter 旋进流量计switching point 切换点symbolic processing 符号处理synaptic plasticity 突触可塑性synergetics 协同学syntactic analysis 句法分析system assessment 系统评价systematology 系统学system homomorphism 系统同态system isomorphism 系统同构system engineering 系统工程tachometer 转速表target flow transmitter 靶式流量变送器task cycle 作业周期teaching programming 示教编程telemechanics 远动学。
doi:10.3969/j.issn.1671-1122.2020.11.001关键信息基础设施安全保护技术体系郭启全1,张海霞2(1.公安部网络安全保卫局,北京 100741;2.中国科学院软件研究所,北京 100190)摘 要:关键信息基础设施安全保护是当前网络空间安全的核心任务。
文章阐述了开展关键信息基础设施安全保护的指导思想,提出了涵盖采集汇聚层、数据治理层、智慧大脑层、业务应用层的技术体系架构,引入大数据分析、人工智能、知识图谱等新型技术,构建网络空间安全地图,利用智慧大脑实现智能化、精准化的情报挖掘、目标画像、行为推理和预测预警,支撑“实战化、体系化、常态化”安全能力建设,为国家网络安全监管部门和重要行业开展关键信息基础设施安全保护工作提供借鉴。
关键词:关键信息基础设施;网络安全;智慧大脑;人工智能;网络空间地图中图分类号:TP309 文献标志码: A 文章编号:1671-1122(2020)11-0001-09中文引用格式:郭启全,张海霞. 关键信息基础设施安全保护技术体系[J].信息网络安全,2020,20(11):1-9.英文引用格式:GUO Qiquan, ZHANG Haixia. Technology System for Security Protection of Critical Information Infrastructures[J]. Netinfo Security, 2020, 20(11): 1-9.Technology System for Security Protection of CriticalInformation InfrastructuresGUO Qiquan1, ZHANG Haixia2(1. Cyber Security Department, The Ministry of Public Security, Beijing 100741, China;2. Institute of Software, Chinese Academy of Sciences, Beijing 100190, China)Abstract: Security assurance of critical information infrastructure is the core work of cyber security. This paper describes the guiding ideology of security assurance of criticalinformation infrastructure. Afterwards, it proposes the technical architecture including thecollection and aggregation layer, data governance layer, intelligent brain layer and businessapplication layer. Technologies such as big data analysis, artificial intelligence and knowledgemap are applied to construct cyber security geographic map, realize intelligent datamining,perform accurate portrait of critical targets, conduct behavior reasoning, provide threatearly-warning, and finally support the construction of practical, systematic and normalizedsecurity abilities. This paper aims to provide the basis for the national cyber securityregulatory authorities and important industries to carry out the security assurance work ofcritical information infrastructures.Key words: critical information infrastructure; cyber security; intelligent brain; artificial intelligence; cyberspace map基金项目:国家重点研发计划[2020YFB1806504]作者简介:郭启全(1962—),男,河北,研究员,硕士,主要研究方向为网络空间安全、网络空间地理学和人工智能;张海霞(1981—),女,河北,高级工程师,博士,主要研究方向为网络空间安全。
In the modern era, smartphones have become an integral part of our daily lives, providing us with a wealth of information and convenience. However, they also come with a significant downside: the proliferation of mobile phone spam. This essay aims to discuss the reasons behind the prevalence of mobile phone spam and suggest some strategies to combat it.Firstly, the widespread use of smartphones has made it easier for spammers to reach a large audience. With billions of users worldwide, mobile phones have become a prime target for advertisers and scammers alike. The anonymity provided by the internet also allows spammers to send out unsolicited messages without fear of immediate consequences.Secondly, the low cost of sending spam messages contributes to the problem. Unlike traditional advertising methods, which can be expensive, sending a spam message via SMS or email is relatively cheap. This low cost encourages spammers to send out a large volume of messages, hoping that a small percentage of recipients will respond.Moreover, the lack of effective regulation and enforcement against mobile phone spam exacerbates the issue. In many countries, there are either no laws or weak regulations in place to combat spam. This lack of legal framework allows spammers to operate with impunity.To address the problem of mobile phone spam, several measures can be taken. Firstly, users should be educated on how to identify and avoid spam messages. This includes not clicking on suspicious links, not providing personal information to unknown sources, and using spam filters on their devices.Secondly, mobile service providers should take a more proactive role in combating spam. They can implement stricter policies on the sending of unsolicited messages and collaborate with law enforcement agencies to identify and prosecute spammers. Thirdly, governments should establish and enforce strong antispam laws. These laws should include penalties for spammers, as well as provisions for compensation for victims of spam. By creating a legal deterrent, governments can discourage potential spammers from engaging in this activity.In conclusion, mobile phone spam is a growing problem that affects millions of users worldwide. By understanding the reasons behind its prevalence and taking appropriate measures, we can work towards a cleaner and safer mobile communication environment.It is essential for individuals, service providers, and governments to join forces in the fight against mobile phone spam.。
AExperimental SetupsThe laboratory equipment that has been employed to obtain the experimental results shown in the book is described in this appendix.In particular,a double tank apparatus and a oven have been used to implement level control and a temperature control tasks,respectively.A.1Level Control ApparatusThe double tank apparatus(made by KentRidge Instruments)adopted for level control experiments is shown in Figure A.1.Although the setup consists of two small perspex tower-type tanks(whose area is A=40cm2),only one at a time has been adopted in the experiments.Each tank isfilled with water by means of a pump whose speed is set by a DC voltage(the manipulated variable),in the range0-5V,through a Pulse Width Modulation(PWM) circuit.The tank isfitted with an outlet at the base in order for the water to return to a reservoir.The measure of the level h of the water is given by a capacitive-type probe that provides an output signal between0(empty tank) and5V(full tank).For the sake of simplicity,the level variable is expressed in Volts.The process can be modelled by the following differential equation:A dhdt=Q i−Q o(A.1)where Q i and Q o are the input(manipulated variable)and outputflow rate respectively.Note that the system is actually nonlinear,since the outputflow rate depends on the square root of the level,i.e.,Q o=a2ghwhere a is the cross sectional area of the outflow orifice and g is the gravita-tional constant.The employed control systems are implemented by means of296A Experimental Setupsa PC-based controller whose sampling time is5ms.It is worth noting that the two tanks(both of them have been employed in the experiments shown in the book)have a different dynamics.Further,different models arise depending on the adopted identification experiment(see Chapter 7).Fig.A.1.The double tank apparatus employed for level control experimentsA.2Temperature Control ApparatusA laboratory scale oven has been employed to implement temperature control tasks.It consists of an aluminium plate that is heated by two resistors attached to it.The plate is inserted in an insulating box(whose dimensions are33×21×16.5cm).A fan(which has not been adopted in the experiments)is present in order to provide a fast cooling of the apparatus.The temperature of the plate is measured by means of a thermocouple.The overall process is sketched in Figure A.2.The same PC-based controller(with a sampling time of5ms)of the level control experiments has been employed.The temperature process can be modelled by the following equations:C p˙τp=P−G pb(τp−τb)C b˙τb=G pb(τp−τb)+G be(τe−τb)(A.2)A Experimental Setups297 whereτp is the temperature of the plate,τb is the temperature of the box,τe is the temperature of the external environment,C p and C c are the heat capacities of the plate and of the box respectively,and G pb and G be are the thermal conductances between the plate and the box and between the box and the external environment,respectively.Finally,P is the thermal power provided by the heating elements.The control task consists of controlling the temperature of the plate by acting on the thermal power of the heating elements,namely,by manipulating the voltage across the resistors.As for the level control task,for the sake of sim-plicity the input and output are expressed in Volts(both in the range0-5V). 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In the realm of future technology,our imaginations can run wild.Heres a detailed English composition that envisions the technological advancements of the future.Title:A Glimpse into the Future of TechnologyAs we stand on the precipice of the next era of technological innovation,it is both thrilling and daunting to consider the potential changes that lie ahead.The future of technology promises to be a tapestry woven with threads of artificial intelligence, quantum computing,biotechnology,and sustainable energy solutions.Artificial Intelligence AIThe integration of AI into daily life will be seamless and ubiquitous.Personal AI assistants will not only manage our schedules and provide information but will also understand our emotions and predict our needs.In the workplace,AI will collaborate with humans to enhance productivity,offering insights and solutions that we might not have considered.Autonomous vehicles will revolutionize transportation,reducing accidents and traffic congestion while optimizing routes for efficiency.Quantum ComputingQuantum computers will unlock new frontiers in data processing and problemsolving. With their ability to perform complex calculations at unprecedented speeds,they will transform fields such as cryptography,drug discovery,and materials science.Quantum encryption will ensure unprecedented security in digital communications,while quantum simulations will enable the design of new materials with tailored properties. BiotechnologyAdvancements in biotechnology will lead to breakthroughs in personalized medicine. Genetic editing technologies like CRISPR will allow us to correct genetic disorders and potentially enhance human capabilities.Synthetic biology will give rise to new forms of life,designed to perform specific functions,such as cleaning up pollution or producing renewable energy.Sustainable EnergyThe quest for sustainable energy will yield innovative solutions to combat climate change. Solar and wind energy will become more efficient and affordable,with advancements in energy storage allowing for a more stable and reliable power grid.Fusion power,once adream of science fiction,may become a reality,providing a nearly limitless and clean source of energy.Virtual and Augmented RealityThe boundaries between the digital and physical worlds will blur as virtual reality VR and augmented reality AR become more sophisticated.VR will offer immersive experiences for entertainment,education,and therapy,while AR will overlay digital information onto the physical world,enhancing our perception and interaction with the environment.Space ExplorationThe future will see a new age of space exploration,with private companies and international collaborations pushing the limits of what we know.Mars may become the first offworld colony,with sustainable habitats and infrastructure built to support human life.Space tourism will become a reality,offering breathtaking views of Earth from the cosmos.CybersecurityAs our reliance on technology grows,so does the importance of cybersecurity.Advanced encryption methods and AIdriven threat detection systems will protect our digital infrastructure from cyber attacks.Quantumresistant algorithms will safeguard our data against the power of quantum computers.Ethical ConsiderationsWith great power comes great responsibility.The future of technology will demand a robust ethical framework to guide its development and use.Issues such as privacy,data ownership,and the digital divide will require thoughtful solutions to ensure that technological advancements benefit all of humanity.In conclusion,the future of technology is a canvas waiting for the brushstrokes of innovation.It holds the promise of a world that is more connected,efficient,and sustainable.However,it also presents challenges that we must navigate with wisdom and foresight.As we step into this future,let us do so with a commitment to using technology for the betterment of all.。
第42卷第11期2020年11月舰船科学技术SHIP SCIENCE AND TECHNOLOGYVol.42,No.11Nov., 2020潜艇隐身技术分析闫大海,张啥,苗金林,杨晓刚(中国舰船研究院,北京100101)摘要:本文分析研究包括声波、电磁波、尾流等在内探测潜艇的主要技术手段,以及针对这些手段,潜艇所采取的包括声隐身、雷达波隐身、尾迹隐身等在内的主要隐身措施。
系统提出探测技术发展趋势。
潜艇隐身技术难度大、涉及专业广,集成度高,需要以需求为牵引,密切跟踪探测技术发展趋势,坚持从设计源头贯彻隐身设计思想,同时不断提高潜艇对不同侦察制导和攻击手段的软硬杀伤能力,探索新技术、新手段,保证我潜艇在现代海战中处于优势地位。
关键词:探测;潜艇;隐身中图分类号:U674文献标识码:A文章编号:1672-7649(2020)11-0128-06doi:10.3404/j.issn,1672-7649.2020.11.026Research on submarine stealth technologyYAN Da-hai,ZHANG Han,MIAO Jin-lin,YANG Xiao-gang(China Ship Research and Development Academy,Beijing100101,China)Abstract:This paper analyzes the main technical ways of detecting submarine,including acoustic wave,electromagnetic wave,wake flow and so on,as well as the main stealth measxires taken for these ways,including acoustic stealth,radar wave stealth,wake stealth and so on.The development trend of detection technology is put forward systematically.The stealth technology of submarines is very difficult,involving a wide range of specialties and high integration.It needs to closely follow the development trend of detection technology,adhere to the stealth design idea from the design source,and constantly improve the soft and hard lethality of submarines to different reconnaissance guidance and attack means,explore new technologies and new means,so as to ensure that our submarines are in an advantageous position in modem naval warfare.Key words:detection;submarine;stealtho引言潜艇的优势在于隐蔽性。
.40中国医疗器械信息 | China Medical Device Information标准检测Standard and T esting鉴于新版国际标准ISO 8637:2010《心血管植入物和体外系统 血液透析器、血液透析滤过器、血液滤过器和血液浓缩器》已发布,且该标准尚未转化成我国新版行业标准,与ISO8637:2004对比,超滤系数已经重新定义且修改了检测方法,本文将对该项目具体检测进行诠释,希望能为国内血液透析器生产厂家对超滤系数的确定提供参考。
如何检测血液透析器超滤系数蓝建华 国家食品药品监督管理局广州医疗器械质量监督检验中心 (广州 510080)内容提要: 目的:探讨新版国际标准ISO 8637:2010中超滤系数的分析检测方案。
方法:计算滤过液流率和跨膜压之间的回归线斜率作为超滤系数。
结论:通过该方案可以确定血液透析器产品的超滤系数。
How to Test Ultrafiltration Coefficient of HaemodialyserLAN Jian-hua Guangzhou Quality Supervision and Iuspection Center for Medical Devices (Guangzhou 510080)Abstract:Objective : To discuss the detection program of ultrafiltration coefficient from ISO 8637:2010. Method : Calculate the ultrafiltrationcoefficient as the slope of the regression line between filtration flow rate and transmembrane pressure. Result : Ultrafiltration coefficient of haemodialyser can be established by the detection program.Key words:ultrafiltration coefficient, transmembrane pressure, filtration flow rate1.实验材料、试剂及设备1.1实验材料空心纤维透析器:低通量透析器和高通量透析器各一支。
不连续介质反演的原对偶牛顿法和全变差正则化冯立新;李媛;张磊【摘要】研究利用散射场测量数据反演非均匀介质的逆散射问题,特别是平面波在非均匀介质中传播时所产生逆散射问题的数值计算.为克服非均匀介质不连续变化和反演具有不适定性的困难,提出基于全变差正则化的原对偶牛顿方法,避免了一般正则化方法对不连续介质交界处反演的过光滑性作用.数值试验显示,本算法可以在观测数据带有一定噪声的境况下有效地重构不连续介质系数.%An inverse scattering problem of inhomogeneous mediums from the measurements of the scattered field is considered.In particular,it focuses on the numerical computation of the inverse scattering generated by the interaction of a plane wave and an inhomogeneous medium.To solve the ill-posedness as well as the difficulties caused by inhomogeneous media,a primal-dual Newton method based on the total variation regularization is constructed.The overly smooth effect of the usual regularization method for the inversion is overcome.Numerical experiments show that this method can recover discontinuous coefficients under moderate amount of noise in the observation data.【期刊名称】《黑龙江大学自然科学学报》【年(卷),期】2018(035)001【总页数】9页(P1-9)【关键词】全变差正则化;原对偶牛顿法;逆介质散射【作者】冯立新;李媛;张磊【作者单位】黑龙江大学数学科学学院,哈尔滨150080;黑龙江大学数学科学学院,哈尔滨150080;黑龙江大学数学科学学院,哈尔滨150080【正文语种】中文【中图分类】O1750 IntroductionIn this paper, we focus on the inverse medium scattering problem of determining electromagnetic properties of unknown inhomogeneous objects embedded in a homogeneous background from noisy measurements of the scattered field corresponding to one incident wave impinged on the objects. We describe the scattering model mathematically as follows:Δu(x)+k2η(x)u(x)=0, x∈R2,(1)where u is the total field, k is the wavenumber, η(x)>0 for all x, andm(x)=1-η(x) is the scatterer with a compact support. We assume that B containing the compact support of the scatterer m(x) be a bounded domain in R2. Let ui which is assumed to satisfyΔui+k2ui=0, x∈R2,(2)denote the incident on the inhomogeneity. Assume that the incident fieldui is a plane wave, i.e., ui(x)=exp(ikd·x), where d∈R2 is the propagation direction (a unit vector). The total field u consists of the incident field ui and the scattered field us, that is,u=ui+us.It follows immediately from Eqs. (1) and (2) that the scattered field satisfies Δus+k2us=k2m(x)ui, x∈R2,(3)and the scattered field is required to satisfy the following Sommerfeld radiation condition(4)uniformly in all directions x/|x|.The inverse medium scattering problems arise naturally in many applications such as geophysical exploration, medical imaging, and radar detection [1-5]. For the practical significance of the inverse problem, some inverse scattering methods have been developed in the literature, which may be divided into two categories: the direct methods and the indirect methods. The direct methods aims at detecting the scatterer support and shape, and includes linear sampling method (LSM)[6-8], factorization method (paper [9], Chapter 5, paper [10]), and multiple signal classification (MUSIC)[11-13]. In contrast, the indirect methods provides a distributed estimate of the refractive index by applying regularization techniques. We just mention recursive linearization [14-18] , Gauss-Newton method [19-21], and level set method [22] for an incomplete list. Generally, theestimates by an indirect method can provide more details of inclusions, but at the expense of increased computational efforts. There has been considerable interest in considering efficient and stable inversion techniques. However, due to the strong nonlinearity of the map from the refractive index to the scattered field, severe ill-posedness of the inverse problem and the limited availability of the scattered data, it is still a very challenging problem.In this work, we assume that the scattered data with fixed wavenumber are known in the domain B, i.e., the scattered field is measured forxj∈B,j=1,…,J for a given incident field. We develop an iterated method for accurately detecting the scatterer support. In the case, from the Lippmann-Schwinger integral equation, the inverse problem can be seen as the operator equation of the first kind with unknown m(x). An efficient numerical method is presented for solving the inverse medium scattering problem which is to reconstruct the inhomogeneous medium from inner measurements of the scattered field. We construct the total variation (TV) regularization approximation of the integral equation. The main reason of choosing TV regularization is that TV can penalize highly oscillatory solutions while allowing jumps in the regularized solution. Consequently, a primal-dual Newton method is used to minimize the TV functional [23-25]. This is an iterated method, which need solve direct scattering problem for each step of the process. The scattering data is generated by numerical solution of the direct scattering problem, which is implemented by using the efficient fast algorithm [26]. In this work, we develop a TVregularization and primal-dual method for solving the inverse medium problem with discontinuous coefficients. The remainder of the paper is organized as follows. Section 1 gives the integral formulation of inverse medium problem (1)~(4) and describes the TV regularization approximation. In Section 2, we employ a primal-dual Newton method for solving the corresponding inverse problem. Section 3 presents the numerical results for the inverse medium problem. Finally, we give the relevant conclusions in Section 4.1 Formulation of the integral equation and TV approximationThe integral formulation of problem (1)~(4) is the main ingredient in the proposed method. Let be the Hankel function of first kind and order 0, see paper [1] for details. We have the following Lippmann-Schwinger integral equation for u:(5)K(x,y)m(y)dy.So, we have following operator equation(Km)(x)=g.Define the Tikhonov-TV functional(6)where TV(m) is the TV of a function m defined on the B. If m is smooth, one can obtain the representation|m|dx.However, the representation is not suitable for the implementation of the numerical procedure, due to the nondifferentiability of the Euclidean norm at the origin. To overcome this difficulty, one can take an approximation to the Euclidean norm |x| like where β is a small positive parameter. This yields the following approximation to TV(m):Instead of the Tikhonov-TV functional (6), we will consider minimization of the functional(7)Suppose m=mi,j is defined on an equispaced grid in two space dimensions, {(x1i,x2j)|x1i=iΔx1,x2j=jΔx2,i=0,…,n1,j=0,…,n2}. We defi ne the discrete penalty functional Jβ(m):R(n1+1)×(n2+1)→R by(8)where To simplify notation, we drop a factor of Δx1Δx2 from the right-hand side of (8). This factor can be absorbed in the regularization α in (7). In the following section, we consider minimization of the discretized functional:(9)where the matrix K is a discretization of the operator K, the vector g and J denote discrete data, and discretization of TV approximation Jβ,respectively.2 A primal-dual Newton methodTo minimize the functional (9), the primal-dual Newton method is employed. Consider the convex functional defined on C=R2. One can show that the conjugate set C* is the unit ball in R2 and corresponding conjugate functional to φβ is(10)We can obtain the dual representation by (10):(11)The following theorem relates the gradient of a convex functional φβ to the gradient of its conjugate see paper [25], p.138 for a proof.Theorem 1 Suppose that φβ is differentiable in a neighborhood ofx0∈C⊂Rd, and the mapping F=gradφβ:Rd→R d is invertible in that neighborhood. Then is Frechét differentiable in a neighborhood ofy0=φβ(x0) withEmploying the dual representation (11), we obtain(12)We stack the array components mi,j,ui,j and vi,j into column vector m,u, and v, let Dx1 and Dx2 be matrix representation for the grid operators and and let <·,·> denote the Euclidean inner product. Then (12) can be rewritten asMinimization of the least squares functional (10) is equivalent to computing the saddle point(u*,v*,m*(13)where We refer to m as the primal variable, and to u and v as the dual variables.Since (13) is unconstrained with respect to m, a first order necessary condition for a saddle point is(14)An additional necessary condition is that the duality gap in (11) must vanish, i.e., for each grid index i, j,(15)Finally, the dual variables must lie in the conjugate set, i.e.,(ui,j,vi,j)∈C*.(16)Suppose (15) holds for a point (ui,j,vi,j) in the interior of C*. ThenUsing Theorem 1, above equations is equivalent toDx1m=B(m)u, Dx2m=B(m)v,(17)where B(m)=diag(1/ψ′(m)).We can reformulate the first order necessary conditions (14) and (17) as a nonlinear system:(18)The derivative of G can be expressed asHere B′(m)u has matrix representationB′(m)u-Dx1=-E11Dx1-E12Dx2(19)withwhere the products and quotients are computed pointwise. Similarly,B′(m)v-Dx2=-E21Dx1-E22Dx2(20)withNewton’s method for the system (18) requires solutions of systems of the formG′(u,v,m)(Δu,Δv,Δm)=-G(u,v,m).Substituting (19)~(20) and app lying block row reduction to convert G′ to block upper triangular form, consequently we obtainwhereandWe employ backtracking to the boundary to maintain the constraint (16). In other words, we computeall i,j}.We then updateAlgorithm Primal-dual Newton’s method for TV functional.ν:=0;m0:=initial guess for primal variable;u0,v0:=initial guess for dual variables;begin primal-dual Newton iterations;Δm:=[KTK+αLν]-1rν;mν+1:=mν+Δm;τν:=max{0≤τ≤1|(uν+τΔu,vν+τΔv)∈C*};uν+1:=uν+τνΔu;vν+1:=vν+τνΔv;ν:=ν+1;end primal-dual Newton iteration.3 Numerical experimentsSome numerical examples are presented to illustrate the performance of the proposed method. Here, the scattering data are generated by numerical solution of the direct scattering problem, which is implemented by using the efficient fast algorithm (see Appendix).In experiments we consider the following inhomogeneities,★ the scattered fields are measured on the domain B=[-2,2]×[-2,2];★ the incident direction d=(cos(π/3),sin(π/3)), and wa ve number k=1;★ {Qi,j⊂R2,i=1,2,…,n1,j=1,2,…,n2} is a partition of B;★ the parameters n1=20(40),n2=20(40), α=0.001, β=0.05.Fig.1 True scatterer (n1)Fig.2 Reconstruction n1 using primal-dual Newton’s methodFig.3 True scatterer (n2)Fig.4 Reconstruction n2 using primal-dual Newton’s methodTo test the stability, some relative random noise is added to the data, i.e., the measurement data takes the formu|B:=(1+δrand)u|B,where ‘rand’ gives the Gaussian white noise and δ is a noise level parameter taken to be 5% in our numerical experiments.We have set the parameter α in the TV formulation. Then, we use the above primal-dual Newton’s algorithm to solve the inverse problem. The stopping criterion for the iteration is a relative decrease of the nonlinear residual by a factor of 10-4 or through 50 times iterations. Here, the initial guess for m can be chosen for different constant. The reconstruction got faster when the the initial guess for m is better. Fig.2 and Fig.4 present reconstruction results of the refractive index from the measurement data. We can see that the method has the ability to resolve the inverse medium problem with discontinuous coefficients efficiently.4 ConclusionsWe have proposed and discussed a reconstruction technique of the inverse medium problem with discontinuous coefficients based on the measurements of the scattering field. Our aim to overcome the difficulties caused by the the ill-posedness as well as the difficulties caused by inhomogeneous media has been realized. To make the discontinuous coefficients of the medium can be reliably reconstructed, we convert the problem to an equivalent optimization problem, and then introduce the regularization term. At the same time, we use primal dual Newton method to solve the above problem. Finally, an inversion algorithm, based on TV regularization, for the inverse medium problem from the measurement data of the scattered field is shown. Numerical experiments show that the method is effective.AppendixHere, we give a fast algorithm to solve forward scattering problem (1)~(4).The method was proposed by Nadaniela Egidi etc, see paper [26] for details. The problem (1)~(4) can be reformulated as a Fredholm integral equation (5) of the second kind:Let {Ql,j⊂R2,l=1,2,…,n1,j=1,2,…,n2} be a p artition of B, the integral equation (5) is discretized as follows:(21)where ξl,j∈R2 is the center of ml,j=m(ξl,j), and ul,j is an approximation of u(ξl,j). Linear system (21) can be rewritten as following formAu=b,where b∈Cn1n2 contains u∈Cn1n2 contains ul, j, and the entry of matrix A, at row corresponding to indices l,j, and at column corresponding to i1, j1, containswhere δ is the Kronecker function.In following we give an approximation of the coefficient matrix A by using the properties of Hankel functions We havewhere J0 is the Bessel function of order 0, and Y0 is the Newmann function of order 0. From the power series expansions of these functions we have tlρ2l, ρ>0,where γ≈0.577 215 7 is the Euler constant, andhere B>0 is a suitable constant that depends on the size of D, and L is a truncation parameter.Substituting above express into (21), we obtain the following linear system:(22)where is the approximation of ul,j .We restrict our attention to coordinate partitions of B, whereQl,j,l=1,…,n1,j=1,…,n2 are given by rectangles having edges parallel to the coordinate axes. Moreover, we use the following notations :Ql,j=[al,bl]×[aj,bj],ξl,j=(ξ1l,ξ2j)∈R2,l=1,…,n1,j=1,…,n2. So, calculating the integral in (22), and rearranging the resulting terms, we obtain-×(-ξ1l)2q+1-l(-ξ2j)2p-2q+1-s)-,l=1,…,n1,j=1,…,n2.(23)Linear system (23) can be solved efficiently due to the special structure of its coefficient matrix, which is given by the identity matrix plus 2(L+1)2 rank-one matrices. We conclude that (23) can be rewritten as follows :(I+UVT)u=b,where U,V are following complex matrices having n1n2 rows and 2(L+1)2 columns.here×(-ξ1,i1)2q+1-l(-ξ2,i2)2p-2q+1-s,i1=1,2,...,n1,i2=1,2,...,n2,M=2L+1,N(l)=2L-2⎣l/2」+1.References[1] COLTON D, KRESS R. Inverse acoustic and electromagnetic scattering theory [M]. Berlin: Springer-Verlag, 1998.[2] CUI T J, CHEW W C, AYDINER A. Inverse scattering of two-dimensional dielectric objects buried in a lossy earth using the distorted Born iterative method [J]. 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Fast detection of system nonlinearity using nonstationary signalsE.Zhang a,Ã,J.Antoni a,R.Pintelon b,J.Schoukens ba University of Technology of Compi e gne,Laboratory Roberval of Mechanics,CNRS UMR6253,Franceb Vrije Universiteit Brussel,Departement ELEC,Pleinlaan2,1050Brussels,Belgiuma r t i c l e i n f oArticle history:Received8July2009Received in revised form26April2010Accepted17May2010Available online1June2010Keywords:Nonlinear systemsNonlinearity detectionNonstationary signalsLocal polynomial methoda b s t r a c tThis paper proposes a method for the detection and quantification of nonlineardistortions in the output of a dynamic system.The basic idea is to use a nonstationaryexcitation that makes the nonlinear distortions also nonstationary,thus makingpossible their differentiation from stationary plant noise.The nonstationarity of theexcitation allows the evolution of the system nonlinearity to be assessed in one singleshot,thus greatly accelerating the experiment.&2010Elsevier Ltd.All rights reserved.1.IntroductionAlmost all practical structures are nonlinear to some extent,the nonlinearity being caused by one or a combination of factors.For instance,visco-elastic mounts show a significant nonlinear behaviour in mechanical engineering and many demountable structures are built with nonlinearities due to loose joints in civil engineering.For these reasons it is an important issue to detect the presence and the level of nonlinear distortions.Is the system under test linear or nonlinear? What is the evolution of the nonlinear distortions present in the system with the shift of excitation level?Haber gives a brief review of nonlinearity tests in Ref.[1],and Vanhoenacker in Ref.[2]summarizes the current techniques for the detection of nonlinearities by means of stationary excitation signals(one excitation level per experiment)such as a sine,a stepped sine,a random stationary signal,or a random-phase multisine signal.However,some of these methods are subject to significant constraints(e.g.they only work on lightly damped systems)and the use of a stationary excitation may be problematic:if too low in level,the induced weak nonlinear distortion is likely to be masked by measurement noise,which would lead the user to make a wrong judgement;if different excitation levels are applied,then the number of experiments will be multiplied accordingly and the whole process may rapidly become excessively time consuming.In this work,a single nonstationary excitation is used to detect nonlinearities in a fast way.The system nonlinearity,as a result of being a function of the nonstationary excitation,is therefore nonstationary too.Assuming the measurement noise to be stationary,the presence of nonlinearities can be distinguished on that basis.However,in the case of a nonstationary excitation,the data analysis involves the estimation of transfer functions and noise variances in a non-steady state that results in the generation of leakage errors due tofinite-length records of non-periodic data.The local polynomial method recently introduced in Refs.[3,4]is adopted here to kick out such errors.Besides,among other current techniques dedicated to nonlinearity detection,the‘‘Fast method’’based on a well designed periodic multisineContents lists available at ScienceDirectjournal homepage:/locate/jnlabr/ymsspMechanical Systems and Signal Processing0888-3270/$-see front matter&2010Elsevier Ltd.All rights reserved.doi:10.1016/j.ymssp.2010.05.011ÃCorresponding author.E-mail address:erliang.zhang@utc.fr(E.Zhang).Mechanical Systems and Signal Processing24(2010)2065–2075signal [5]–steady state measurements –will serve as a point of reference to validate the results of the proposed nonstationary approach.In this perspective,a special signal is designed based on a multisine structure with a random harmonic grid with nonstationary periods.Being periodic (on the long term)and nonstationary (within each period)at the same time,such a signal will be found not only useful to compare both methods,but also to achieve a separation of the nonlinear distortions from the measurement noise.The paper is organised into three parts.In the first part,the problem is stated in the output-error framework in which noise is assumed only at the output measurements.In the second part,the approach using a nonstationary excitation is first presented in combination with the Fast method and then in combination with the local polynomial method.Numerical and laboratory experiments are then introduced in the third part to demonstrate the validity of the proposed approach.2.Problem statementFor the sake of simplicity,the single-input single-output (SISO)case will be considered throughout,although the proposed methodology is trivially generalized to the multiple-input multiple-output (MIMO)case.A nonlinear system G will be modelled as the sum of its underlying best linear approximation (BLA)G BLA plus a remaining error called the ‘‘stochastic nonlinear part’’[6].The input–output relationship,in the discrete-time setting,will then be described asy ðt Þ¼G BLA ðq Þu ðt Þþy s ðt Þþy n ðt Þ¼y BLA ðt Þþy s ðt Þþy n ðt Þð1Þwhere q is the shift operator,u (t )is the excitation to the system,G BLA is the underlying BLA of the nonlinear system defined by minimizing the distance y (t )ÀG (q )u (t )in the least square sense,y s (t )is the stochastic nonlinear part that depends on the power spectrum and the probability distribution of the excitation,and y n (t )is the plant noise modelled as y n (t )=H (q )e (t )with e (t )a white noise process and H (q )a shaping filter.For a sampled signal x (t ),measured at t =0,1,y ,N À1,the discrete Fourier transform (DFT)will be defined asX ðk Þ¼1ffiffiffiffiN p X NÀ1t ¼0x ðt Þe Àj 2p kt =N :ð2ÞThen,the equivalent input–output relationship to Eq.(1)in the DFT domain isY ðk Þ¼G BLA ðO k ÞU ðk ÞþT Y BLA ðO k ÞþY s ðk ÞþT Y S ðO k ÞþY N ðk ÞþT Y N ðO k Þ¼G BLA ðO k ÞU ðk ÞþT ðO k ÞþV ðk Þð3Þwhere O k ¼e jk o s =N with o s the sampling frequency,T (O k )=T Y BLA (O k )+T Y S (O k )+T Y N (O k )is a generalized transient term that accounts for the leakage errors 1in the linear and nonlinear parts of the plant and in the noise dynamics,respectively [7],and where the output noise V (k )=Y S (k )+Y N (k )accounts for the contribution of the stochastic nonlinear distortions and the measurement noise,respectively.Under mild assumptions it can be generally assumed that,owing to the DFT mechanism,the spectrum Y N (k )of the measurement noise is asymptotically (N -N )normally distributed;the same assumption holds for the spectrum Y S (k )of the system nonlinearity under the class of Gaussian excitations [5].These assumptions are desirable,yet not necessary in the proposed method.The detection and the quantification of Y S (k )in Eq.(3)with respect to the level of the excitation U (k )is the main focus of the present work.3.Techniques for the detection of system nonlinearityIn this section,the so-called ‘‘Fast method’’of Ref.[5]is first briefly reviewed to serve as a reference point for the new approach using a nonstationary excitation signal,which is presented next.3.1.Review of the Fast methodThe Fast method has proven very reliable to detect system nonlinearities.It relies on the use of a specially designed input T -periodic signal,called multisine,with a random harmonic grid:u ðt Þ¼X F k ¼1A k cos ðk o 0t þf k Þ,ð4Þwhere o 0=2p /T is the fundamental frequency,F is the number of frequency lines,{A k }are user-defined amplitudes,and{f k }are phases that can be chosen as independent realizations of an uniformly distributed random process on [0,2p )such that e f e j f k g ¼0with e fg the expected value.The signal u (t )has a Gaussian-like distribution over time for large F and is in general spectrally coloured according to the selection of amplitudes {A k }.The key point for nonlinearity detection is to1Let P N (t )be the rectangular window that selects samples t =0,y ,N À1in a signal.Then,if two signals u (t )and v (t )are related as v (t )=L (q )u (t )with L (q )a linear filter,the leakage error is defined as the difference DFT{v (t )P N (t )}–L (O k )ÁDFT{u (t )P N (t )}between the DFT of the truncated output and the DFT of the truncated input times the filter frequency response.It is an ‘‘end-effect’’error,whose inverse DFT corresponds to transients at the onset and end edges of P N (t ).It decreases as an O (1/N ).E.Zhang et al./Mechanical Systems and Signal Processing 24(2010)2065–20752066design signal u (t )so that it excites only a well chosen set of frequency lines.A full grid of frequency lines is first generated according to Eq.(4),then groups of L (Z 2)consecutive lines are collected into blocks,and finally one frequency line is dropped randomly (A k =0)from each block so as to form a random harmonic grid as depicted in Fig.1.The set of excited lines,{o k :A k a 0},will be noted I .Of prime importance at this juncture is the observation that nonlinear systems respond at additional harmonics (not in I )resulting from various combinations of positive and negative excited frequencies.Therefore,the inspection of the system response at non-excited lines allows the detection,qualification,and quantification of nonlinear distortions.In practice,care is taken to record data once the plant transient terms T Y BLA þT Y S in Eq.(3)have disappeared.Plant transient-effects,and consequently leakage-errors,can therefore be eliminated.As for the measurement noise its presence will be inevitable,and it will interfere with the detection of the nonlinear distortions at non-excited frequency lines in the output.The measurement noise can however be assessed from one single experiment due to the fact that multiple periods are measured.Indeed,the sample mean and sample variance over P periods can be calculated by synchronous averaging as follows:^Y ðk Þ¼1P X P p ¼1Y ½p ðk Þ,s2Y N ðk Þ¼1P À1X Pp ¼1ðY ½p ðk ÞÀ^Y ðk ÞÞðY ½p ðk ÞÀ^Y ðk ÞÞð5Þwhere the overline denotes the complex conjugate and Y [p ](k )the DFT corresponding to the p th period of the excitationsignal as illustrated in Fig.3a.The synchronous averaged measurement ^Ynormally contains only responses of the BLA and nonlinear distortions for P large enough.After the measurement noise being removed in this way,the spectrum of ^Ycan be used to detect the presence of nonlinear distortions.The Fast method will be used hereafter to validate the new approach based on the design of a nonstationary excitation signal discussed in the next paragraph.3.2.The proposed method using a nonstationary excitation signal3.2.1.Principle of the nonstationary methodThe motivation for using a nonstationary signal for nonlinearity detection is twofold.First,this quite elegantly turns the difficult task of distinguishing the presence of nonlinear distortions from measurement noise in the system output,as described by Eq.(1),into the much easier task of checking the presence of nonstationarity.Indeed,if measurement noise y n (t )can be reasonably assumed stationary,then the only reason why the output noise v (t )=y n (t )+y s (t )may evidence nonstationarity is precisely because the system produces a nonlinear distortion y s (t ).Second,a nonstationary excitation signal has the definite advantage of gradually driving the system outside its linear range,thus making possible the appraisal of its nonlinearity degree as a function of the excitation level in one single shot.Fig.2illustrates the components of the measured response of a nonlinear system excited by a nonstationary excitation with an instantaneous increasing root-mean-square (RMS).The design of a nonstationary excitation signal is,in general,a trivial task.However,for the purpose of comparison with the Fast method which is pursued in this paper,one requires the nonstationary signal to be also periodic with a random harmonic grid.As shown in the previous section,another advantage of having a periodic signal is the possibility of separating the stochastic nonlinear noise from the measurement noise.A periodic excitation signal with a nonstationary behaviour within one period (and random harmonic grid)is illustrated in Fig.3.Each period of the signal is further divided into N S segments which have N S /2different excitation levels.Whereas the Fast method applies on a full period (Fig.3a),Fig.1.Basic principle of the Fast method.The second row illustrates the construction of a random harmonic grid by randomly removing frequency lines in all consecutive groups of L lines of a full harmonic grid (first row).The last row depicts the spectral response of a nonlinear system,with energy produced at non-excitedlines.Fig.2.Original idea to detect the nonlinear distortions using the nonstationary signal.E.Zhang et al./Mechanical Systems and Signal Processing 24(2010)2065–20752067the nonstationary method uses the measurements corresponding to each segment inside a period (Fig.3b):on each segment a local BLA and a local output noise V are estimated,whose evolutions then permit the investigation of the system nonlinearity.It happens that the constraint of having a random harmonic grid somewhat complicates the design of such a signal,which cannot be obtained simply by repetition of a single nonstationary period.The next subsection proposes an iterative algorithm that alleviates this problem by alternatively imposing the nonstationarity constraint in the time domain and the random harmonic grid constraint in the frequency domain until convergence is reached.3.2.2.Generation of a nonstationary periods with a random harmonic gridThis subsection describes how to design a periodic signal with nonstationary periods and a random harmonic grid I .The iterative design algorithm is as follows:(1)Specify an instantaneous RMS envelope RMS 0(t )that features the nonstationarity of the signal over one period T (e.g.steadily increasing and then decreasing amplitude in time with slopes 72ffiffiffi3p =T ,the slopes so calculated as to conserve unit energy of the signal —see the black lines in Fig.4a.(2)Generate a random-phase multisine with constant amplitude A ,period T ,unit RMS value and a random harmonic grid,from Eq.(4).(3)A period of the signal,denoted u i (t )at this step,is further divided into a user-defined number segments;the RMS valueis calculated for each segment and then interpolated between segments with cubic splines to obtain the new RMS envelope RMS i (t ).The ratio RMS 0(t )/RMS i (t )denotes the difference between the desired shape and that of the i th iteration signal;it is used as a scale-factor to produce the new signal periodu i þ1ðt Þ¼u i ðt ÞRMS 0ðt ÞRMS i ðt Þ:ð6ÞFast methodNonstationary methodp periodsN sG BLA,1V ,1G BLA,3V ,3u [1]u [2]Fig.3.(a)Periodic signal for the Fast method and (b)additional division into N S segments within each period for the nonstationary method.1234567−10010Time (s)u (t )5001000150020002500−400−2000200Frequency (Hz)Frequency (Hz)U (d B )U (d B )381382383384385386387388389390−400−2000200Fig.4.(a)Arrow-shaped excitation signal (L =3),(b)its spectrum,and (c)an enlarged partial view showing the imposed random harmonic grid.E.Zhang et al./Mechanical Systems and Signal Processing 24(2010)2065–20752068(4)The DFT U i+1(k)=A i+1(k)e j f iþ1kðÞof u i+1(t)is computed according to Eq.(2),where A i+1(k)and f i+1(k)denote themagnitude and the phase of the k th line at the i+1step;the random harmonic grid with constant amplitude is then forced to be~Uiþ1ðkÞ¼Ae j f iþ1kðÞk2I0k=2I(ð7Þand the modified~U iþ1(k)is transformed back into the time domain.(5)Repeat steps(3)–(4)until the ratio RMS0(t)/RMS i(t)converges to unity.The convergence of the algorithm can be justified as follows.Eq.(6)is a linear transformation from u i(t)to u i+1(t) wherein the factor RMS0(t)/RMS i(t)is certainly less than or equal to1for at least one part of the signal u i(t).According to the contraction mapping2theorem[8],this part of the signal will converge to a unique solution.On the other hand,the modification in Eq.(7)also helps to the convergence of the iterative algorithm by keeping the desired spectrum of the signal.The number of design variables{f k},i.e.the number of excited frequency lines should not be too small for the iteration algorithm to work effectively.Fig.4illustrates the result of the algorithm after300iterations.As can be seen,the period of the signal correctly complies with the imposed nonstationary RMS envelope,whilst at the same time its spectrum has the imposed random harmonic grid where only frequency lines in a given set I have been excited.3.2.3.Removal of leakage errors with the local polynomial methodNo plant leakage errors will be introduced when an integer number of periods of the signal designed in Section3.2.2is analyzed.However,since the time-varying behaviour of the excitation within one period is to be used for the detection of nonlinear distortions,the analysis must be performed on segments of one full period,as depicted in Fig.3b.This certainlycauses the presence of plant leakage errors T YBLA þT YSin any segment,which may mask the presence of nonlineardistortions in the output noise and therefore jeopardise our approach.Nevertheless,leakage errors in the frequency domain have a smooth nature that can be taken advantage of to be modelled and thus extracted together with the BLA, G BLA,by a local polynomial curve-fitting which is described next[9].Let us denote G BLA as G for simplicity.Thanks to the smooth behaviour of G and T¼T YBLA þT YSþT YN,the following Taylorseries(up to order R+1)holds at frequency lines k+r,with r¼0,71,...,7n and n the number of measurement points, GðO kþrÞ¼GðO kÞþX Rs¼1g sðkÞr sþOððr=NÞðRþ1ÞÞTðO kþrÞ¼TðO kÞþX Rs¼1t sðkÞr sþNÀ1=2Oððr=NÞðRþ1ÞÞ:ð8ÞArranging all terms G(O k),T(O k),and the coefficients of the Taylor series g s,t s,s¼1,...,R in a row vector Y and their respective powers in a column vector K(k,r),the insertion of Eq.(8)into Eq.(3)yieldsYðkþrÞ¼Y Kðk,rÞþVðkþrÞð9Þwith Y(k+r),V(k+r)defined in Eq.(3)and K(k,r)dependent on U(k).Collecting a series of equations for r¼Àn,Ànþ1,...,0,...,nfinally yields the matrix equationY n¼Y K nþV nð10Þwith Y n2C1Âð2nþ1Þ,K n2C2ðRþ1ÞÂð2nþ1Þ,and V n2C1Âð2nþ1Þconstructed by stacking the values of Y(k+r),K(k,r),and V(k+r) from left to right.Solving Eq.(10)in the least-square sense eventually yields the polynomial estimate of^Y,i.e.^Y¼Yn K HnðK n K HnÞÀ1.The residue of the least-squaresfit,^V n,is then^Vn¼Y nÀ^Y K n¼Y n P n,with P n¼I2nþ1ÀK H nðK n K H nÞÀ1K nð11Þand it is related to the noise V n as^V n¼V n P n with P n an idempotent matrix.Hence,an estimate of the noise variance s2V is given by^s2VðkÞ¼1d ^Vn^V Hn,with d¼2nþ1À2ðRþ1Þð12Þwhere d=rank(P n)is the number of the degrees of freedom of the residual^V n.It is noteworthy that the estimator^s2V embodies two contributions,thefirst one stemming from the measurement noise and the second one from the nonlinear distortions.Since the variance^s2V is estimated over2n+1frequencies–the true 2Let S be a subspace of a normed space X and let T:S-S be a transform from S to S.Then T is a contraction mapping if there is an a with0r a r1such that99T(x)ÀT(y)99r a99xÀy99for x,y A S.Here,x stands for u i,T(x)for u i+1as given by Eq.(6),and a for RMS0/RMS i.E.Zhang et al./Mechanical Systems and Signal Processing24(2010)2065–20752069variance s 2V ðk þr Þis implicitly assumed equal to s 2V ðk Þfor r =Àn ,Àn +1,y ,0,y ,n in Eq.(12)–this introduces an interpolation error O (n /N ).As the value n is lower-bounded by R –see Eq.(12)–it is necessary to choose R not too large.The three other estimation errors affecting ^s 2V are the polynomial interpolation error O ((n /N )2R +2)of the transfer function,the residual leakage error O ((n /N )R +2)and O ((n /N )2R +3)that depends on both the plant and noise dynamics,respectively,and which decrease as R grows.A good compromise is R =2.Sometimes n is chosen larger to get a better noise rejection,this resulting in a smoother estimate for ^s 2V over frequency.More details about these bias errors can be found in Ref.[8].For the purpose of demonstration and before tackling the more difficult nonlinear case,a simulation example is provided here to illustrate the ability of the local polynomial method to reduce leakage errors in estimating the transfer function of a linear system in comparison with the classical WOSA estimator (weighted overlapped segment averaging),i.e.the transfer function estimated as the ratio of the averaged cross and autoperiodograms [10].In this example,a filtered Gaussian noise is used to excite a linear system H 0=A (q )/B (q )(whose parameters are given in the footnote 3).The measurements are purposely noiseless so that leakage errors are the only disturbances in the estimation of the transfer function.The length of the full measurement record is 213.For the local polynomial method,R =2,n =3are used to estimate H loc ,and for the window method,a Hanning window is used with 8segments and 50%overlap to estimate H win .Fig.5clearly shows the superior ability of the local polynomial method to reduce leakage errors on the transfer function estimation of a linear system.This excellent capability for leakage rejection will obviously apply as well in the case of a nonlinear system in order to remove T (k )in Eq.(3),and thus allow an unambiguous detection of the output noise V (k )that contains the nonlinear distortions.3.2.4.Treatment of the errors-in-variables problem by a simple strategyIt is worth pointing out that the local polynomial method presented so far applies in the output-error framework only.However,in practice the measured input (excitation force)is always contaminated by measurement noise as well.As a consequence,matrix K n in Eq.(10)will be contaminated with errors,thus,leading to biased estimates of the transfer function and of the noise covariance matrix.In addition,with the increase of the excitation level,the amplifiers,transducers,and other equipments will probably make the input/output measurement noise slightly nonstationary.This may interfere with our initial fundamental assumptions on the stationarity of the output measurement noise,and may prevent us from distinguishing and thus detecting the evolution of nonlinear distortions from that of measurement noise.A simple strategy to overcome these difficulties is to make use of the periodic property of the input signal designed in Section 3.2.2,so as to remove noise by synchronous averaging as was done by Eq.(5)in Section 3.1with the Fast method.This allows not only to decrease the bias of the estimators ^Yand ^s V caused by the input measurement noise,but also to separate the output measurement noise from the nonlinear distortions in the output.Following the notation of Eq.(5),let y [p ](t )and u [p ](t )denote the p th period of signals y (t )and u (t ).Then,the following synchronous averages are calculated:y ¼1XP p ¼1y p ½ ,u ¼1XP p ¼1u p ½ :ð13ÞIf enough periods P are measured and provided the input and output measurement noises are not coherent from one period to another,y and u will converge to their expected values according to the law of large numbers.The input and output measurement noises can be subtracted from the measurements based on Eq.(13).The subtracted measurement noises are also divided into N S segments as done for the excitation signal.The measurement noises of each segment are transformed into the frequency domain via Eq.(2)where they asymptotically follow a zero complex circular distribution,and thus their variances are easily estimated in the same way as Eq.(5).As the nonlinear distortions in the output are perfectly coherent from one period to another,they thus remain in the output y after the output measurements being averaged by Eq.(13).The averaged input u and output y are used for the local polynomial method to estimate the row vector Y .The response of the BLA of a nonlinear system and the leakage errorNormalized frequencyA m p l i t u d e (dB )parison of estimated transfer functions (line:true transfer function H 0,circles:9H 0ÀH win 9,points:9H 0ÀH loc 9).3a =[0.0493,0.0986,0.0593],b =[1,À1.7599,0.9571].E.Zhang et al./Mechanical Systems and Signal Processing 24(2010)2065–20752070are calculated as ^Y¼^Y K n ;furthermore,the response of the BLA at the k th frequency line is estimated as ^Y 1,1½ ðk ÞK n ,1,n þ1½ ðk Þwhere the index [i ,j ]indicates the position of a selected element.Finally,the nonlinear distortions can be detected according to Eq.(11)and quantified by Eq.(12).4.ApplicationsIn this section,the effectiveness of using a nonstationary excitation combined with the local polynomial method for the detection of system nonlinearity is first demonstrated on a simulated example and then on an actual mechanical structure.4.1.Simulation caseThe proposed methodology is demonstrated here on a Wiener–Hammerstein system which,as illustrated in Fig.6,consists of a cascade of a linear time-invariant (LTI)system G 1(q )=A 1(q )/B 1(q ),a static polynomial nonlinearity modelled as s (t )=ap 2(t )+bp 3(t ),and another LTI system G 2(q )=A 2(q )/B 2(q ).All polynomial coefficients,A 1,B 1,A 2,B 2,and coefficients a ,b of the nonlinearity are provided 4.The sampling frequency f s is 104Hz.The output y further is disturbed by a filtered Gaussian noise with standard deviation 0.1(see Fig.6).The noise filter H (q )is a second order discrete-time low-pass Butterworth filter with cut-off frequency 8000Hz.After having designed a nonstationary period of 217samples with a random harmonic grid according to the algorithm of Section 3.2.2,the signal period is repeated P =33times so as to form a periodic input u (t ).The response of the Wiener–Hammerstein system to that excitation is then measured,and the first two periods are discarded in order to decrease transient effects —note this is only needed for the Fast method,the nonstationary approach being able to kick transients out thanks to the local polynomial method outlined in Section 3.2.3.One period is used for the local polynomial method with R =2and n =3,whose results are then compared with those of the Fast method based on P À2periods.The output noise V (k )estimated by both methods is shown in Fig.7.It is found that both methods agree very well with each other.It should be remembered that at this stage V (k )includes the contributions of both the measurement noise and the nonlinear distortions.Extraction of the latter from the former could be achieved on the basis of the synchronous averages described in Section 3.2.4,yet it is not pursued in this example.Making use of the nonstationarity of the excitation signal,it is further possible to follow the evolution of the system nonlinearity as a function of the excitation level.For that,the full period of the signal is divided into N S =16segments,each segment having a different excitation level for the first-half period as illustrated in Fig.3.The evolution of the system nonlinearity with the increase of the excitation level is thus investigated in one single experiment.In this case n =8is chosen in the local polynomial method –see Eq.(10)–to smooth the output noise over frequency lines in order to visualize it clearly for different excitation levels.But this is done at the cost of increasing the interpolation error on the estimation of the output noise V.Fig.6.Wiener–Hammerstein system.Frequency (Hz)E s t i m a t e d t r a n s f e r f u n c t i o n (d B )E s t i m a t e d o u t p u t n o i s e s (d B )Fig.7.Estimated BLA transfer function at the excited frequencies (left axis)and output noise V (k )(right axis)(diamonds:local polynomial method and circles:Fast method).4LTI 1:b =[1],a =[0.95,À1.4,0.9];LTI 2:b =[1,0.5],a =[0.95,À0.9,0.9].Nonlinear part:a =1e–3,b =1e–5.E.Zhang et al./Mechanical Systems and Signal Processing 24(2010)2065–20752071。