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    • 7. 发明申请
    • Method for Estimating Transmission Properties of a Telecommunications Transmission Line
    • 估计电信传输线传输特性的方法
    • US20120163559A1
    • 2012-06-28
    • US13394392
    • 2009-09-11
    • Antoni FertnerPer Ola BörjessonDaniel Cederholm
    • Antoni FertnerPer Ola BörjessonDaniel Cederholm
    • H04B3/46
    • H04B3/466
    • Transmission properties of a telecommunications transmission line may be estimated with improved accuracy by numerical solution for Γ of Zin·jω̂C=Γcoth(Γ). At least one curve is adapted to Γ solutions already obtained and a starting point for numerical solution is selected in dependence of the at least one curve and in dependence of an already obtained solution close in frequency. In a first frequency range, starting points for numerical solution may be calculated from a biquadratic equation. In a second frequency range, a line in the complex plane may be adapted to solutions already obtained and new starting points selected in dependence of the line and in dependence of the previous solution. In a third frequency range, two lines in the frequency plane may be adapted to solutions already obtained and new starting points selected in dependence of the lines.
    • 电信传输线路的传输特性可以通过&Ggr的数值解决方案提高精度来估计; 的Zin·jωC=&Ggr; coth(&Ggr。)。 至少有一条曲线适应于&Ggr; 已经获得的解决方案和数值解的起点根据至少一条曲线选择,并且依赖于已经获得的频率接近的解。 在第一个频率范围内,数值解的起始点可以从二次方程计算。 在第二频率范围中,复平面中的线可以适应已经获得的解和根据线选择并且依赖于先前解的新起始点。 在第三频率范围内,频率平面中的两条线可以适应已经获得的解和根据线选择的新起点。
    • 9. 发明授权
    • Transmission line parameter determination
    • 传输线参数确定
    • US09470729B2
    • 2016-10-18
    • US14110215
    • 2011-04-08
    • Fredrik LindqvistPer Ola BörjessonAntoni Fertner
    • Fredrik LindqvistPer Ola BörjessonAntoni Fertner
    • G01R27/02H04B3/466
    • G01R27/02H04B3/466
    • The present disclosure relates to determining parameters in a model of a transmission line. For determining the parameters, reflection coefficient defining data and the total capacitance of the transmission line are obtained. Further, true reflection coefficients obtained through the reflection coefficient defining data are applied in an objective function for the line. The objective function for the line is a sum of error signals and each error signal is the difference between a model value of a reflection coefficient and a corresponding true reflection coefficient. Further, the objective function is minimized by utilizing gradients of the objective function with respect to the transmission line parameters to be determined. A capacitive length is employed and at least two further transmission line parameters are determined as combinations of a basic resistive transmission line parameter, a basic capacitive transmission line parameter and a basic inductive transmission line parameter of the transmission line model.
    • 本公开涉及确定传输线的模型中的参数。 为了确定参数,获得反射系数定义数据和传输线的总电容。 此外,通过反射系数定义数据获得的真实反射系数被应用于该行的目标函数中。 线的目标函数是误差信号的和,每个误差信号是反射系数的模型值和相应的真实反射系数之间的差。 此外,通过利用待确定的传输线参数的目标函数的梯度来最小化目标函数。 使用电容长度,并且将至少两个另外的传输线参数确定为传输线模型的基本电阻传输线参数,基本电容传输线参数和基本感应传输线参数的组合。
    • 10. 发明授权
    • Method for transmission line analysis
    • 传输线分析方法
    • US08385510B2
    • 2013-02-26
    • US13129555
    • 2009-11-27
    • Miguel BergDaniel CederholmKlas EricsonPer Ola Börjesson
    • Miguel BergDaniel CederholmKlas EricsonPer Ola Börjesson
    • H04M1/24H04M3/08H04M3/22
    • H04B3/46H04M3/306H04M11/062
    • A FDR SELT measurement is made in a stop band of a DSL band plan, using a PSD allowed by the PSD mask. Further measurements may also be made in an adjacent pass band and further bands, and the results combined to create a wide-band measurement result. When transformed into the time domain (e.g. by inverse Fourier transform to produce the line impulse response) greater resolution in time (and hence greater spatial resolution) is achieved. In order to compensate for AGC calibration errors measurements using different AGC steps may be scaled to fit smoothly to each other. If measurements overlap, measurement results in the region of overlap may be combined in various ways to limit the influence of noise and to create a smooth transition from one measurement to the next.
    • 使用PSD掩模允许的PSD,在DSL频段计划的停止频段进行FDR SELT测量。 还可以在相邻通带和另外的带中进行进一步测量,并且结果组合以产生宽带测量结果。 当变换到时域(例如通过逆傅立叶变换产生线脉冲响应)时,可以获得更高的时间分辨率(因此更大的空间分辨率)。 为了补偿AGC校准误差,使用不同AGC步长的测量可以被缩放以相互平滑地相配合。 如果测量重叠,重叠区域中的测量结果可以以各种方式组合,以限制噪声的影响并创建从一个测量到下一个测量的平滑过渡。