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    • 106. 发明专利
    • DETECTING DEVICE FOR NEGATIVE ELECTRIC CHARGE IN THE AIR
    • JPH10153578A
    • 1998-06-09
    • JP35173696
    • 1996-11-22
    • TOMONAGA KATSUHIDE
    • KITAMURA SHIGENOBU
    • G01R29/24G01N27/60
    • PROBLEM TO BE SOLVED: To obtain a device by which the existence of static electricity of negative electric charge in the air is detected as one standard to know the cleanliness of the air inside a room, which is low-cost, and which is small-sized so as to be put into a pocket. SOLUTION: The side of the gate 9 of a field-effect transistor(FET) is connected to metal body (a plate, a rod or a net), for negative-electric-charge sensing, in a required size, the side of the source 8 of the field-effect transistor 10 is connected to a ground via an input resistance 17 and a switching circuit 6, the switching circuit 6 is connected to the anode side of a power supply 12 via a light-emitting diode 2 for negative-electric-charge display and a control resistance 15, the cathode side of the power supply 12 is connected to the ON- side terminal 18 of a switch 5, the switch 5 is in a grounded state when it is set to the OFF side, and the metal body 1 for sensing is connected to its OFF-side terminal 19 via a protective resistance 4 and a protective diode 3.
    • 107. 发明专利
    • STANDARD SAMPLE FOR MEASURING SPACE CHARGE, AND METHOD OF MEASURING SPACE CHARGE
    • JPH09311122A
    • 1997-12-02
    • JP12724796
    • 1996-05-22
    • FUJIKURA LTD
    • YOKOYAMA AYAKOMIYATA HIROYUKI
    • G01R29/24G01N1/00G01N27/60
    • PROBLEM TO BE SOLVED: To provide a standard sample capable of regularly providing stable distribution of space charge and accumulated quantity of space charge by providing electrodes formed of a pair of conductors opposite to a body formed of a ceramic sintered body. SOLUTION: Circular thin plate-like electrode parts 3, 3 formed of a pair of conductors are provided on both surfaces of a body 2 formed of ceramic sintered body which constitutes a standard sample 1 so as to be opposed thereto. As the material forming the body 2, a ceramic sintered body dielectric body generally used as ceramic capacitor which is a dielectric body having the performance of almost scattering the space charges accumulated in the body 2 by voltage application by grounding is preferred. For example, a sintered body of titanium oxide is used. As the conductors forming the electrodes 3, 3, aluminum, gold and the like are used. The diameter of the standard sample 1 is set to 100-120mm, and the thickness (t) of the standard sample 1 (body 2) corresponding to the space between the electrode parts 3, 3 is set to 1-3mm. The electrode parts 3, 3 have diameters of 20-40mm and thicknesses (a), (a) of 1.0-3.0mm.
    • 109. 发明专利
    • MEASURING APPARATUS FOR ELECTRIFICATION AMOUNT
    • JPH09138217A
    • 1997-05-27
    • JP31967595
    • 1995-11-13
    • RICOH KK
    • IIMURA HARUO
    • G01R29/24G01N27/60
    • PROBLEM TO BE SOLVED: To obtain a measuring apparatus by which the saturation electrification amount and the saturation time of a sheetlike or filmlike sample are measured efficiently without hardly damaging the sample to be measured. SOLUTION: A measuring apparatus is composed of a sample plate 3 in which a sample layer 2 is formed so as to come into contact on a conductive substrate 1, of a sample-plate holding member 4 which holds the sample plate 3, of a roller 5 which is installed so as to come into contact with the sample plate 2, of a sample-plate movement mechanism 6 which moves the sample-plate holding member to a direction perpendicular to the tangent line of the roller 5 to the sample layer 2 and of an electric-charge measuring device 7 which measures the electric charge amount of the sample plate 3. The sample plate 3 is moved back and forth by the sample-plate movement mechanism 6, it is repeatedly brought into contact with, and separated from, the roller 5, and an electric charge which is generated in the sample layer 2 is measured by the electric-charge measuring device 7.
    • 110. 发明专利
    • DEVICE FOR DETECTING ELECTRIC CHARGE
    • JPH0980099A
    • 1997-03-28
    • JP23848495
    • 1995-09-18
    • MATSUSHITA ELECTRONICS CORP
    • MASUYAMA MASAYUKIMATSUDA YUJI
    • G01R31/26G01R29/24G01R31/319H01L21/66
    • PROBLEM TO BE SOLVED: To improve charge detection sensitivity of a device for detecting electric charge. SOLUTION: A charge detection part 2 made of an N-type impurity layer on a P-type impurity semiconductor substrate 1 accumulates electric charge. Voltage fluctuation of the charge detection part 2 is electrically transmitted to the gate electrode of a drive transistor part 6 and output as charge of source potential VO of the drive transistor part 6. Here, the source potential VO of the drive transistor part 6 is electrically transmitted to the gate electrode of a feedback transistor part 8 disposed between the drain electrode of the drive transistor part 6 and a power source part VOD through a voltage shift part 9. Thus, since the drain potential of the drive transistor part 6 trails displacement of potential (namely, gate potential of drive transistor 6) of the charge detection part 2 by the feedback transistor part 8, the junction capacitance between the gate and the drain of the drive transistor 6 is small, the whole capacitance of the charge detection part 2 is decreased and charge detection sensitivity is improved.