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    • 2. 发明专利
    • ULTRASONIC FLOW-VELOCITY MEASURING APPARATUS
    • JPH10170318A
    • 1998-06-26
    • JP33180796
    • 1996-12-12
    • OSAKA GAS CO LTDKANSAI GASMETER KK
    • OKAMURA SHIGENORIIKADA TAKAOMITOMITA AKIOKONO AKIOKOBAYASHI SHUNYASUDA TETSUYA
    • G01P5/00G01F1/66
    • PROBLEM TO BE SOLVED: To obtain an ultrasonic flow-velocity measuring apparatus in which phases of reflected ultrasonic waves are put in order so as to acquire coherent received waves and whose measuring accuracy can be ensured sufficiently by a method wherein an oval-shaped measuring part is formed inside a measuring pipe and transducers are arranged and installed in both focal positions of it. SOLUTION: An oval-shaped body shell 7 is installed in a measuring part 1a inside an ultrasonic flow-velocity measuring pipe 1, and transducers 2, 3 are arranged and installed in both focal positions of it. When ultrasonic waves are transmitted from a transmitting element at the transducer 2, a part of the ultrasonic wave reaches a receiving element at the transducer 3 as rectilinear propagation waves. However, the greater part of the ultrasonic waves are reflected only once by the inside wall of the oval-shaped body shell 7 so as to reach the receiving element at the transducer 3 in the focal position on the other side in the same time. Consequently, received waves which are output from an amplifier circuit 5 are changed into coherent waves in which phases are put in order and in which the reflected ultrasonic waves are overlapped. Then, a changeover circuit 6 is changed over, ultrasonic waves are transmitted from the transducer 3, and coherent waves are output from the circuit 5 in the same manner. Consequently, it is possible to obtain the measuring pipe 1 whose measuring accuracy can be ensured sufficiently.
    • 4. 发明专利
    • ULTRASONIC FLOW VELOCITY MEASURING METHOD
    • JPH09318644A
    • 1997-12-12
    • JP13164496
    • 1996-05-27
    • OSAKA GAS CO LTDKANSAI GASMETER KK
    • OKAMURA SHIGENORIIKADA TAKAOMITOMITA AKIOKONO AKIONAKAMURA EIJI
    • G01P5/00G01F1/66G01S11/14
    • PROBLEM TO BE SOLVED: To surely determine the received wave arrival timing and measure the flow velocity with high accuracy by integrating the waves of one or both polarities of the received waves, and setting the time when the integrated output reaches the reference value to the received wave arrival timing for measuring the propagation time difference. SOLUTION: Received waves from transceivers 2, 3 are half-wave shaped by a half-wave shaping circuit 7 through an amplifying circuit 5, and the integrated output from an integrating circuit 8 is compared with the reference voltage from a reference voltage generating circuit 10 by a comparing circuit 9. The reference voltage is set to the middle value where the integrated output rises synchronously with the rise of the half wave of the second wave, thus the integrated output reaches the reference voltage value at the middle time when it rises along the rise of the second wave beyond the peak value of the first wave, and the received wave arrival signal is outputted from the comparing circuit 9 at this time. When the received signal is integrated, the integrated output can be increased in response to the received wave-form, and the first wave of the received wave is not required to be captured.
    • 8. 发明专利
    • ULTRASONIC FLOW VELOCITY MEASURING METHOD
    • JPH1038650A
    • 1998-02-13
    • JP19236096
    • 1996-07-22
    • OSAKA GAS CO LTDKANSAI GASMETER KK
    • OKAMURA SHIGENORIIKADA TAKAOMITOMITA AKIOKONO AKIONAKAMURA EIJIYASUDA TETSUYA
    • G01P5/00G01F1/66
    • PROBLEM TO BE SOLVED: To secure sufficiently high measuring accuracy by surely recognizing the first half wave of received waves by forming the first wave of a driving pulse impressed upon an ultrasonic transmitting element in a triangular wave which rises gently and falls steeply. SOLUTION: The first wave P1 of a driving pulse P outputted from a pulse generating circuit is formed in a triangular wave which rises gently P11 and falls steeply P12 . Consequently, the waveform of the received wave which is received by means of and outputted from a receiver becomes that of the received wave W shown in the figure. Namely, the first half wave W1 of the received wave W corresponding to the steeply falling section P12 of the triangular wave P1 becomes such a waveform that becomes the highest at the peak value and descends after the peak value. Accordingly, when, for example, the half wave W1 is not able to be caught, because the reference level for measuring propagating time difference fluctuates and exceeds the peak value of the half wave W1 of the received wave W1 no output is generated. Therefore, the measuring accuracy of an ultrasonic flow rate measuring method can be secured, because the measurement can be discriminated as invalid and the possibility of catching the second half wave W2 and waves after the half wave W2 is eliminated.
    • 9. 发明专利
    • METHOD OF ULTRASONIC MEASURING FLOW VELOCITY
    • JPH1019619A
    • 1998-01-23
    • JP16911596
    • 1996-06-28
    • OSAKA GAS CO LTDKANSAI GASMETER KK
    • OKAMURA SHIGENORIIKADA TAKAOMITOMITA AKIOKONO AKIONAKAMURA EIJI
    • G01P5/00G01F1/66G01S11/14
    • PROBLEM TO BE SOLVED: To enhance the precision of flow velocity measurement by monitoring the peak value in a received wave and controlling the amplitude value of the received wave so that the peak value is constant for each received wave. SOLUTION: A transmitted wave is transmitted from a transmitter-receiver 2 on the upstream side of a fluid and received by a transmitter-receiver 3 on the downstream side. The integrated output of an integrating circuit 8 is compared with the reference voltage of a reference voltage generating circuit 10 by a first comparing circuit 8, and when the integrated output reaches a reference voltage value, a spare signal is outputted. On the other hand, the received wave amplified by an amplifying circuit 5 is compared with zero volt by a second comparing circuit 11, and a zero cross signal is outputted. The spare signal and the zero cross signal are inputted to an AND circuit 12, which then outputs a received wave arrival signal, and determines the received wave arrival timing. A control circuit 14 monitors the output value of a peak hold circuit 13, and controls the amplifying circuit 5 to minimize the amplified value in the amplifying circuit 5 when the output value is increased, and to increase it when the output value is minimized.