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    • 2. 发明授权
    • Buoy
    • 浮标
    • US07900571B2
    • 2011-03-08
    • US12090837
    • 2006-10-18
    • Barry N. JaberAlan WignallJohn D. Martin
    • Barry N. JaberAlan WignallJohn D. Martin
    • B63G8/14
    • B63B22/003B63B22/18
    • A buoy is provided with first and second fixed hydrodynamic surfaces (15,16). When the buoy is towed through water by a tether (17), the first hydrodynamic surface (15) generates a downward force that reduces with increased speed through the water. The second hydrodynamic surface (16) generates an upward force that increases with increased speed through the water so that the buoy dives up to an upper critical speed through the water speed and rises beyond said upper critical speed through the water. The downward force of the first hydrodynamic surface (15) overcomes the buoyancy of the buoy at a lower critical speed through the water above, which the buoy dives. The hydrodynamic surface (15) comprises first fins (15) mounted on an outer casing (1) of the buoy and are spaced angularity and extend parallel to the center axis of the buoy which is substantially aligned with the direction of towing. The second hydrodynamic surface (16) comprises second fins (16) mounted on the outer casing arranged upstream of the first fins (15) in the direction of towing. The second hydrodynamic surface (16) is set at an angle of incidence such that it creates a stalled flow condition at said upper critical speed through the water.
    • 浮标设置有第一和第二固定流体动力表面(15,16)。 当浮标通过绳索(17)拖过水时,第一流体动力表面(15)产生向下的力,其通过水的速度增加而减小。 第二流体动力表面(16)产生向上的力,其随着通过水的速度增加而增加,使得浮标通过水速度达到上临界速度并且通过水升高超过所述上临界速度。 第一流体动力表面(15)的向下的力通过浮标潜水的上面的水,以较低的临界速度克服浮标的浮力。 流体动力学表面(15)包括安装在浮标的外壳(1)上的第一散热片(15),并且与浮子的中心轴线平行地间隔开并且与拖曳方向基本对齐。 第二流体动力学表面(16)包括安装在外壳上的第二翅片(16),其沿着牵引方向布置在第一翅片(15)的上游。 第二流体动力表面(16)被设置成入射角,使得其在所述上临界速度下通过水产生停滞的流动状态。
    • 3. 发明申请
    • BUOY
    • 浮标
    • US20090149092A1
    • 2009-06-11
    • US12090837
    • 2006-10-18
    • Barry N. JaberAlan WignallJohn D. Martin
    • Barry N. JaberAlan WignallJohn D. Martin
    • B63B22/18
    • B63B22/003B63B22/18
    • A buoy is provided with first and second fixed hydrodynamic surfaces (15,16). When the buoy is towed through water by a tether (17), the first hydrodynamic surface (15) generates a downward force that reduces with increased speed through the water. The second hydrodynamic surface (16) generates an upward force that increases with increased speed through the water so that the buoy dives up to an upper critical speed through the water speed and rises beyond said upper critical speed through the water. The downward force of the first hydrodynamic surface (15) overcomes the buoyancy of the buoy at a lower critical speed through the water above, which the buoy dives. The hydrodynamic surface (15) comprises first fins (15) mounted on an outer casing (1) of the buoy and are spaced angularity and extend parallel to the centre axis of the buoy which is substantially aligned with the direction of towing. The second hydrodynamic surface (16) comprises second fins (16) mounted on the outer casing arranged upstream of the first fins (15) in the direction of towing. The second hydrodynamic surface (16) is set at an angle of incidence such that it creates a stalled flow condition at said upper critical speed through the water.
    • 浮标设置有第一和第二固定流体动力表面(15,16)。 当浮标通过绳索(17)拖过水时,第一流体动力表面(15)产生向下的力,其通过水的速度增加而减小。 第二流体动力表面(16)产生向上的力,其随着通过水的速度增加而增加,使得浮标通过水速度达到上临界速度并且通过水升高超过所述上临界速度。 第一流体动力表面(15)的向下的力通过浮标潜水的上面的水,以较低的临界速度克服浮标的浮力。 流体动力学表面(15)包括安装在浮标的外壳(1)上的第一散热片(15),并且与浮子的中心轴线平行地间隔开并且与拖曳方向基本对齐。 第二流体动力学表面(16)包括安装在外壳上的第二翅片(16),其沿着牵引方向布置在第一翅片(15)的上游。 第二流体动力表面(16)被设置成入射角,使得其在所述上临界速度下通过水产生停滞的流动状态。