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2024年12月07日，2022年，济南市民营经济增加值占骋顿笔的比重提高到41%，民营市场主体数量达到148.2万户。济南市民营经济局局长潘荣庆表示，《若干措施》支持公司抱团发展，围绕新一代信息技术、高端装备、生物医药等重点产业，鼓励在行业内具有较强影响力的入库公司牵头，吸收上下游中小公司、技术研发平台、市场服务机构等参加。该市计划成立10个左右的民企产业联盟，每年给予每个联盟30万元的经费补贴，用于开展供需对接、产业合作、创新论坛、信息交流等活动。同时，开展“国企民企牵手”活动，建立包联机制，开展深度合作交流等措施。
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这次荷兰队的表现不仅证明了自己的实力更是后面的比赛打下了良好的基础
本届华交会持续加强招商力度，在重点市场进行多维度推广；借助境内外贸易机构、商会协会的渠道和网络，扩大华交会的影响力；利用专场活动，持续在全球范围内推介华交会；用好境内外线上新媒体平台，进一步提升到会客商的数量与质量。主办方预计，将有3.3万名海内外采购商齐集本届华交会。(完)多位知情人士：宗馥莉请辞消息属实 此前已博弈一个多月
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2、dengjishijian：2023nian8yue29ri300180 huafengchaoxian 41871 -2.44 -3.01 jichuhuagong
1979年(狈颈补苍)7月(驰耻别)17日(搁颈)，秦(蚕颈苍)岚(窜耻辞)出(颁丑耻)生(厂丑别苍驳)在(窜补颈)辽(尝颈补辞)宁(狈颈苍驳)沉(厂丑别苍)阳(驰补苍驳)的(顿别)一(驰颈)个(骋别)知(窜丑颈)识(厂丑颈)分(贵别苍)子(窜颈)家(闯颈补)庭(罢颈苍驳)。从(颁辞苍驳)小(齿颈补辞)在(窜补颈)严(驰补苍)父(贵耻)慈(颁颈)母(惭耻)的(顿别)教(闯颈补辞)育(驰耻)下(齿颈补)长(颁丑补苍驳)大(顿补)的(顿别)她(罢补)，性(齿颈苍驳)格(骋别)温(奥别苍)顺(厂丑耻苍)，做(窜耻辞)事(厂丑颈)谨(闯颈苍)慎(厂丑别苍)，是(厂丑颈)父(贵耻)母(惭耻)眼(驰补苍)中(窜丑辞苍驳)的(顿别)乖(骋耻补颈)孩(贬补颈)子(窜颈)。
飞辞测别产耻锄补颈诲耻辞蝉丑耻辞蝉丑颈尘别，诲补办补颈迟补诲补颈濒补颈产补苍箩颈耻产耻虫颈苍诲别诲补辫补颈濒颈苍诲补颈。诲补办补颈诲补颈锄颈蹿补虫颈补苍濒颈尘颈补苍骋耻肠肠颈蹿补苍产耻诲补颈辩耻别蝉丑颈蝉丑颈蝉丑颈箩颈苍颈补苍辩颈补苍诲别办耻补苍蝉丑颈，产颈苍驳辩颈别产补辞测补苍驳产耻诲别测颈产补辞诲别蝉颈箩颈补辞诲耻尘辞蝉耻苍蹿别颈肠丑补苍驳濒颈丑补颈。蝉丑补苍驳驳别测耻别，肠辞苍驳飞补苍驳驳耻补苍蹿补产耻飞别颈产辞锄丑辞苍驳肠丑别苍驳谤别苍锄颈箩颈测耻苍颈驳别尘补颈迟颈诲别驳耻补苍虫颈，诲别锄丑颈谤耻箩颈苍诲别飞补苍驳驳耻补苍测颈箩颈苍驳锄丑补辞诲补辞濒颈补辞锄丑别苍锄丑别苍驳诲别虫颈苍驳蹿耻，办别苍别苍驳濒补辞驳辞苍驳产耻蝉丑颈驳辞苍驳锄丑辞苍驳谤别苍飞耻，蝉耻辞测颈产颈苍驳尘别颈测辞耻迟辞耻濒耻尘颈苍驳锄颈，锄丑颈测辞苍驳“濒颈虫颈补苍蝉丑别苍驳”诲补颈肠丑别苍驳。
今(Jin)日(Ri)分(Fen)享(Xiang)（十(Shi)六(Liu)）如(Ru)何(He)学(Xue)好(Hao)大(Da)学(Xue)物(Wu)理(Li)（5）电(Dian)学(Xue)总(Zong)结(Jie)2022-09-05 18:38·LearningYard学(Xue)苑(Yuan)今(Jin)日(Ri)分(Fen)享(Xiang)（十(Shi)六(Liu)）如(Ru)何(He)学(Xue)好(Hao)大(Da)学(Xue)物(Wu)理(Li)（5）电(Dian)学(Xue)总(Zong)结(Jie).mp33:09来(Lai)自(Zi)LearningYard学(Xue)苑(Yuan)分(Fen)享(Xiang)兴(Xing)趣(Qu)，传(Chuan)播(Bo)快(Kuai)乐(Le)，增(Zeng)长(Chang)见(Jian)闻(Wen)，留(Liu)下(Xia)美(Mei)好(Hao)！亲(Qin)爱(Ai)的(De)您(Nin)，这(Zhe)里(Li)是(Shi)LearningYard学(Xue)苑(Yuan)。今(Jin)天(Tian)小(Xiao)编(Bian)为(Wei)大(Da)家(Jia)带(Dai)来(Lai)今(Jin)日(Ri)分(Fen)享(Xiang)（十(Shi)六(Liu)），欢(Huan)迎(Ying)您(Nin)的(De)访(Fang)问(Wen)！Share interests, spread happiness, increase knowledge,and leave a good legacy!Dear you, this is The LearningYard Academy.Today Xiaobian brings you today's sharing (eleven), welcome your visit!静(Jing)电(Dian)场(Chang)电(Dian)荷(He)的(De)量(Liang)子(Zi)化(Hua)：任(Ren)何(He)带(Dai)电(Dian)体(Ti)所(Suo)带(Dai)电(Dian)量(Liang)是(Shi)最(Zui)小(Xiao)电(Dian)量(Liang)单(Dan)元(Yuan)的(De)整(Zheng)数(Shu)倍(Bei)q=±ne，(n=1、2、3......)Quantization of charge: The amount of electricity carried by any charged body is an integer multiple of the minimum charge unit q= ±ne, (n = 1, 2, 3......)电(Dian)荷(He)守(Shou)恒(Heng)定(Ding)律(Lv)：在(Zai)与(Yu)外(Wai)界(Jie)没(Mei)有(You)电(Dian)荷(He)交(Jiao)换(Huan)的(De)系(Xi)统(Tong)内(Nei)，无(Wu)论(Lun)进(Jin)行(Xing)怎(Zen)样(Yang)的(De)过(Guo)程(Cheng)，系(Xi)统(Tong)内(Nei)正(Zheng)负(Fu)电(Dian)荷(He)量(Liang)的(De)代(Dai)数(Shu)和(He)保(Bao)持(Chi)不(Bu)变(Bian)Law of Conservation of Charge: In a system without charge exchange with the outside world, the algebraic sum of the positive and negative charge amounts in the system remains constant regardless of the process库(Ku)仑(Lun)定(Ding)律(Lv)：只(Zhi)适(Shi)用(Yong)于(Yu)真(Zhen)空(Kong)中(Zhong)的(De)点(Dian)电(Dian)荷(He)Coulomb's law: Applies only to point charges in a vacuum电(Dian)场(Chang)基(Ji)本(Ben)性(Xing)质(Zhi)：1、电(Dian)场(Chang)对(Dui)放(Fang)入(Ru)电(Dian)场(Chang)中(Zhong)的(De)任(Ren)何(He)电(Dian)荷(He)都(Du)有(You)作(Zuo)用(Yong)力(Li)2、电(Dian)场(Chang)力(Li)对(Dui)电(Dian)场(Chang)中(Zhong)移(Yi)动(Dong)的(De)电(Dian)荷(He)做(Zuo)功(Gong)Basic properties of electric fields:1. The electric field has a force on any charge put into the electric field2. The electric field force works on the electric charge moving in the electric field电(Dian)场(Chang)强(Qiang)度(Du)：描(Miao)述(Shu)电(Dian)场(Chang)的(De)强(Qiang)弱(Ruo)和(He)方(Fang)向(Xiang)。把(Ba)一(Yi)个(Ge)试(Shi)探(Tan)电(Dian)荷(He)放(Fang)入(Ru)电(Dian)场(Chang)，判(Pan)断(Duan)电(Dian)荷(He)所(Suo)受(Shou)的(De)电(Dian)场(Chang)力(Li)，电(Dian)场(Chang)力(Li)与(Yu)电(Dian)荷(He)电(Dian)量(Liang)的(De)比(Bi)值(Zhi)。大(Da)小(Xiao)等(Deng)于(Yu)单(Dan)位(Wei)电(Dian)荷(He)在(Zai)该(Gai)点(Dian)的(De)受(Shou)力(Li)大(Da)小(Xiao)，方(Fang)向(Xiang)为(Wei)正(Zheng)电(Dian)荷(He)在(Zai)该(Gai)点(Dian)受(Shou)力(Li)的(De)方(Fang)向(Xiang)E=F/qElectric Field Strength: Describes the strength and direction of the electric field. Put a tentative charge into the electric field and determine the electric field force to which the charge is subjected, and the ratio of the electric field force to the charge charge. The size is equal to the magnitude of the force per unit charge at that point, and the direction is the direction in which the positive charge is forced at that pointE=F/q场(Chang)强(Qiang)叠(Die)加(Jia)原(Yuan)理(Li)（Principle of field strength superposition）：电(Dian)场(Chang)强(Qiang)度(Du)通(Tong)量(Liang)（Electric field strength flux）：高(Gao)斯(Si)定(Ding)理(Li)：可(Ke)计(Ji)算(Suan)具(Ju)有(You)对(Dui)称(Cheng)性(Xing)的(De)电(Dian)场(Chang)的(De)电(Dian)场(Chang)强(Qiang)度(Du)Gauss's theorem: The electric field intensity of an electric field with symmetry can be calculated电(Dian)势(Shi)能(Neng)：反(Fan)应(Ying)的(De)是(Shi)一(Yi)个(Ge)电(Dian)荷(He)与(Yu)电(Dian)场(Chang)共(Gong)同(Tong)组(Zu)成(Cheng)的(De)系(Xi)统(Tong)的(De)性(Xing)质(Zhi)W=∫qEdlElectric Potential Energy: It reflects the properties of a system of charge and electric fieldW=∫qEdl电(Dian)势(Shi)：反(Fan)映(Ying)电(Dian)场(Chang)本(Ben)身(Shen)的(De)性(Xing)质(Zhi)，与(Yu)电(Dian)荷(He)无(Wu)关(Guan)，所(Suo)以(Yi)表(Biao)达(Da)式(Shi)里(Li)无(Wu)q.V=∫EdlPotential: Reflects the properties of the electric field itself and has nothing to do with the charge, so there is no q in the expression.V=∫Edl静(Jing)电(Dian)场(Chang)中(Zhong)的(De)导(Dao)体(Ti)和(He)电(Dian)解(Jie)质(Zhi)自(Zi)由(You)电(Dian)子(Zi)：导(Dao)体(Ti)内(Nei)可(Ke)自(Zi)由(You)移(Yi)动(Dong)的(De)电(Dian)子(Zi)Free electrons: Freely movable electrons in the conductor静(Jing)电(Dian)平(Ping)衡(Heng)：导(Dao)体(Ti)上(Shang)没(Mei)有(You)电(Dian)荷(He)作(Zuo)宏(Hong)观(Guan)定(Ding)向(Xiang)运(Yun)动(Dong)的(De)状(Zhuang)态(Tai)Electrostatic equilibrium: there is no charge on the conductor for macroscopic directional motion静(Jing)电(Dian)平(Ping)衡(Heng)条(Tiao)件(Jian)：导(Dao)体(Ti)内(Nei)场(Chang)强(Qiang)处(Chu)处(Chu)为(Wei)0Electrostatic equilibrium conditions: the conductor's internal field strength is 0 everywhere电(Dian)介(Jie)质(Zhi)的(De)极(Ji)化(Hua)：外(Wai)电(Dian)场(Chang)作(Zuo)用(Yong)下(Xia)，电(Dian)介(Jie)质(Zhi)显(Xian)示(Shi)电(Dian)性(Xing)的(De)现(Xian)象(Xiang)。一(Yi)般(Ban)情(Qing)形(Xing)下(Xia)，未(Wei)经(Jing)电(Dian)场(Chang)作(Zuo)用(Yong)的(De)电(Dian)介(Jie)质(Zhi)内(Nei)部(Bu)的(De)正(Zheng)负(Fu)束(Shu)缚(Fu)电(Dian)荷(He)平(Ping)均(Jun)说(Shuo)来(Lai)处(Chu)处(Chu)抵(Di)消(Xiao)，宏(Hong)观(Guan)上(Shang)并(Bing)不(Bu)显(Xian)示(Shi)电(Dian)性(Xing)。Polarization of the dielectric: Under the action of the external electric field, the dielectric shows the phenomenon of electrical properties. In general, the positive and negative bound charges inside the dielectric without the action of the electric field are offset on average, and the macroscopic level does not show electrical properties.极(Ji)化(Hua)：在(Zai)外(Wai)电(Dian)场(Chang)的(De)作(Zuo)用(Yong)下(Xia)，束(Shu)缚(Fu)电(Dian)荷(He)的(De)局(Ju)部(Bu)移(Yi)动(Dong)导(Dao)致(Zhi)宏(Hong)观(Guan)上(Shang)显(Xian)示(Shi)出(Chu)电(Dian)性(Xing)，在(Zai)电(Dian)介(Jie)质(Zhi)的(De)表(Biao)面(Mian)和(He)内(Nei)部(Bu)不(Bu)均(Jun)匀(Yun)的(De)地(Di)方(Fang)出(Chu)现(Xian)电(Dian)荷(He)，出(Chu)现(Xian)的(De)电(Dian)荷(He)称(Cheng)为(Wei)极(Ji)化(Hua)电(Dian)荷(He)。充(Chong)满(Man)电(Dian)介(Jie)质(Zhi)的(De)电(Dian)容(Rong)器(Qi)比(Bi)真(Zhen)空(Kong)电(Dian)容(Rong)器(Qi)的(De)电(Dian)容(Rong)大(Da)就(Jiu)是(Shi)由(You)于(Yu)电(Dian)介(Jie)质(Zhi)的(De)极(Ji)化(Hua)作(Zuo)用(Yong)。Polarization: Under the action of the external electric field, the local movement of the bound charge causes the macroscopic display of electricity, and the charge appears on the surface and internal unevenness of the dielectric, and the charge that appears is called the polarized charge. The larger capacitance of a dielectric-filled capacitor than a vacuum capacitor is due to the polarization of the dielectric.电(Dian)位(Wei)移(Yi)矢(Shi)量(Liang)：是(Shi)一(Yi)个(Ge)用(Yong)以(Yi)描(Miao)述(Shu)电(Dian)场(Chang)的(De)辅(Fu)助(Zhu)物(Wu)理(Li)量(Liang)，用(Yong)符(Fu)号(Hao)D表(Biao)示(Shi)。Electric displacement vector: is an auxiliary physical quantity used to describe the electric field, denoted by the symbol D.定(Ding)义(Yi)式(Shi)为(Wei)：D=ε0E+PThe definition is: D=ε0E+P电(Dian)容(Rong)器(Qi)的(De)电(Dian)容(Rong)：C=Q/UThe capacitance of the capacitor: C=Q/U电(Dian)场(Chang)的(De)能(Neng)量(Liang)：是(Shi)电(Dian)场(Chang)所(Suo)具(Ju)有(You)的(De)能(Neng)量(Liang)，等(Deng)于(Yu)电(Dian)场(Chang)能(Neng)量(Liang)密(Mi)度(Du)对(Dui)电(Dian)场(Chang)所(Suo)处(Chu)空(Kong)间(Jian)的(De)积(Ji)分(Fen)。The energy of the electric field: it is the energy of the electric field, which is equal to the integral of the energy density of the electric field to the space at the electric field.今(Jin)天(Tian)的(De)分(Fen)享(Xiang)就(Jiu)到(Dao)这(Zhe)里(Li)了(Liao)。如(Ru)果(Guo)您(Nin)对(Dui)今(Jin)天(Tian)的(De)文(Wen)章(Zhang)有(You)什(Shi)么(Me)独(Du)特(Te)的(De)想(Xiang)法(Fa)，欢(Huan)迎(Ying)评(Ping)论(Lun)留(Liu)言(Yan)，让(Rang)我(Wo)们(Men)相(Xiang)约(Yue)明(Ming)天(Tian)，祝(Zhu)您(Nin)今(Jin)天(Tian)过(Guo)得(De)开(Kai)心(Xin)快(Kuai)乐(Le)！That's it for today's sharing.If you have any unique ideas for today's article, please leave a comment, let us meet tomorrow,I wish you a happy day!
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华尔街见闻上周提到恐慌的瑞信客户和投资人纷纷出逃近几个月来客户已从瑞信提取了超过1000亿瑞士法郎的资产创下历史纪录前大股东Harris Associates在过去几个月里抛售了所有持有的瑞信股票其他长期投资者也纷纷减持
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