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    • 2. 发明授权
    • Electrophoretic separation
    • 电泳分离
    • US5106468A
    • 1992-04-21
    • US814381
    • 1985-12-30
    • Robert J. L. Chimenti
    • Robert J. L. Chimenti
    • B01D57/02C10G32/02
    • B01D57/02C10G32/02Y10S204/08Y10S204/09
    • For the electrophoretic separation of a dispersed phase or contaminant (solid, liquid, or gaseous) from a continuous liquid phase under conditions of intrinsic ionic conductivity due to intrinsic bipolar ions in the continuous phase, especially for conductivities of the continuous liquid phase in excess of about 10.sup.-8 (.OMEGA..m).sup.-1 for which known electrofiltration processes are relatively ineffective or unworkable, a voltage is applied to the dispersed phase-containing liquid phase. The dispersed phase has a field-dependent mobility, and the applied voltage is such as to establish, within the liquid to be treated, a periodic asymmetric electric field E(t), conveniently comprising alternate positive and negative rectangular pulses, having the properties that the time-averaged amplitude of E(t) over one complete period, T, is zero but the average amplitude of each positive feature of the periodic waveform is unequal to that of each negative feature. These conditions give rise to a net electrophoretic migration of dispersed phase which causes dispersed phase to accumulate in a collection region, for example on one or more collector surfaces or within the liquid bulk. In the former case, the collector surfaces are periodically cleaned or regenerated (for deposited solids) or, for liquid or gaseous contaminants, the dispersed phase separates by settling or floatation from the collector surfaces. In the latter case the collected dispersed phase can be mechanically filtered off (with a solid dispersed phase) or allowed to settle or float (for solid, liquid or gaseous dispersed phases). The process is of particular practical importance for the electrofiltration of contaminated petroleum liquids.
    • 对于在连续相中由于本征双极离子导致的本征离子导电性条件下,连续液相的分散相或污染物(固体,液体或气体)的电泳分离,特别是连续液相的电导率超过 约10-8(OMEGA.m)-1,其中已知的电渗过程相对无效或不可行,向分散相含有液相施加电压。 分散相具有场依赖性的迁移率,并且所施加的电压使得在待处理液体内建立周期性不对称电场E(t),其方便地包括交替的正矩形脉冲和负矩形脉冲,具有如下特性: E(t)在一个完整周期T的时间平均振幅为零,但周期波形的每个正特征的平均振幅不等于每个负特征的平均振幅。 这些条件引起分散相的净电泳迁移,其导致分散相积聚在收集区域中,例如在一个或多个收集器表面上或在液体体积内。 在前一种情况下,收集器表面被周期性地清洁或再生(用于沉积的固体),或者对于液体或气体污染物,分散相通过从收集器表面沉降或漂浮而分离。 在后一种情况下,收集的分散相可以机械过滤掉(具有固体分散相)或允许沉降或漂浮(用于固体,液体或气体分散相)。 该过程对于污染的石油液体的电渗滤特别重要。
    • 5. 发明授权
    • Separation of dispersed phase from phase mixture
    • 分散相与相混合物分离
    • US4624763A
    • 1986-11-25
    • US601275
    • 1984-04-17
    • Robert J. L. Chimenti
    • Robert J. L. Chimenti
    • B01D11/04B01D17/02B03C5/02C10G73/28C02F1/48C10G33/02
    • C10G73/28B01D11/04B01D17/0217B03C5/024
    • In order to separate dispersed contaminant phase from a phase mixture comprising the contaminant phase dispersed in a continuous background fluid phase (for example a water-in-oil emulsion), net unipolar charge is injected into the emulsion with an electrostatic charge injection device (1) which issues charged phase mixture into a separation vessel (6). The injected charge both induces an electric field within the embodiment in vessel (6) and also charges the water droplets, resulting in migration of contaminants within the phase mixture in a conglomeration region (33) of the vesssel (6). The mean inter-contaminant spacing is less than, and preferably very much less than (e.g. less than 1%), the smallest internal dimension of the separation vessel so that some conglomeration will occur within the liquid mixture and some will occur on the inner wall surface region of the separation vessel (6). The water droplets settle out to form a distinct water layer (38) on the bottom of the separator vessel (6). The separation effectiveness may be assisted by a bed of closely packed beads (32) occupying a further conglomeration region (34 ) within the separation vessel.
    • 为了将分散的污染物相与包含分散在连续背景液相(例如油包水乳剂)中的污染物相的相混合物分离,用静电电荷注入装置(1)将净单极电荷注入乳液中 ),其将带电相混合物发射到分离容器(6)中。 注入的电荷都在容器(6)的实施例中引起电场,并且还对水滴进行充电,导致在容器(6)的集聚区域(33)内的相混合物内的污染物迁移。 平均污染物间距小于,优选非常小于(例如小于1%),分离容器的最小内部尺寸,使得在液体混合物内将发生一些聚集,并且一些将发生在内壁上 分离容器(6)的表面区域。 水滴沉淀出,在分离器容器(6)的底部形成一个不同的水层(38)。 分离效果可以通过占据分离容器内另外的聚集区域(34)的紧密填充的珠子(32)的床来辅助。
    • 7. 发明授权
    • Detection of uranium by light induced luminescence
    • 通过光诱导发光检测铀
    • US4236071A
    • 1980-11-25
    • US40900
    • 1979-05-21
    • Robert J. L. Chimenti
    • Robert J. L. Chimenti
    • G01N21/64G01V8/02G01V5/00
    • G01N21/6408G01N21/64G01V8/02
    • A method for the detection and identification of uranium bearing materials in media found in nature such as rocks, soils, surface and sub-surface waters, vegetation, or in material which has been subjected to physical or chemical processing comprises the steps of: irradiating the media with a light, having a single wavelength or narrow band of wavelengths in the range of about 2400 to 5000A for a time equal to or less than about 100 microseconds; waiting for a period of time, which is dependent on twice the distance of the light-source to the irradiated medium, followed by measurement of the intensity and decay time of the luminescent light emitted by the irradiated media in a narrow spectral range, having a wavelength greater than the wavelength of the light used to irradiate the media. The method is useful for remote geochemical prospecting for uranium using laser induced luminescence and in monitoring products and effluents from installations processing or utilizing uranium compounds, such as in elemental or isotopic separation, purification, recovery and ore beneficiation.
    • 用于检测和识别在自然界中发现的介质中的铀轴承材料的方法,例如岩石,土壤,表面和地下水,植被或经过物理或化学处理的材料的方法包括以下步骤: 具有光的介质,具有在约2400至5000A范围内的单个波长或窄波长波段等于或小于约100微秒; 等待一段时间,这取决于光源与被照射介质的距离的两倍,随后测量在窄光谱范围内由照射介质发射的发光的强度和衰减时间,其具有 波长大于用于照射介质的光的波长。 该方法可用于使用激光诱导发光的铀远程地球化学勘探,以及监测来自安装处理或利用铀化合物的产品和废水,如元素或同位素分离,纯化,回收和选矿。