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electrical rechenvorrichtung to solution of mathematical differential equations

机译:电微分方程解

摘要

754,113. Electric analogue calculating apparatus. ASSOCIATED ELECTRICAL INDUSTRIES, Ltd. Aug. 12, 1953 [Aug. 28, 1952], No. 21658/52. Class 37. An electric analogue computing apparatus for solving differential equations representing physical problems comprises a resistance network representing at least part of the equation in finite difference form and having a series of nodal junction points representing successive position points of the difference equation, together with means for feeding currents to the junction points and for measuring the resulting voltages thereon by comparison of such voltages with required voltage values satisfying the problem to be solved, so as to derive error signals from the nodal junction points which are simultaneously displayed in a visual array so that the effect of input adjustments upon the voltage relationships at individual nodal junction points may be determined. Fig. 1 shows a section of a resistor analogue network for solving the 4th order differential equation defining the critical speeds of a whirling shaft where x is a position along the shaft; y is the shaft deflection; E is Young's modulus; I is the moment of inertia about the shaft axis; m is the weight of shaft per unit length; # is the critical speed; which network comprises resistance chains N1, N2 comprising resistances R1, R2 and interconnected by resistances R3; the values of resistances R1, R2, R3 being determined by local values of E, I and m with appropriate scaling factors. Nodal points An, Bn represent the n'th of a series of positional points measured along the shaft axis dividing it into sections corresponding to successive network meshes. Current In from point Cn is fed through resistance R4 into point Bn of chain N1 and a voltage Un measured with reference to the network zero point appears at point An of chain N2 to represent the shaft deflection y. The value of In is adjustable, and for the solution of equation (1) where α is a scaling constant; #xSP1/SP,#xSP11/SP are intervals of x to the left and right of the shaft point represented by An, Bn; #n is a constant bearing reaction at this shaft point, so that the voltage drop Pn across R4 is given by where Un, Pn are measured voltages; bn is a known constant; ao is a constant multiple of #SP2/SP for each network mesh at solution; and during the iterative adjustment of successive networks towards solution where Qn is a residual error-signal. Fig. 2 shows a device for systematic iterative adjustment of the network during which Qn#0 and a#ao for each nodal point, wherein the current In supplied to each nodal point Bn is derived from an alternating source V over an adjusting variable resistance Rx and the series resistance R4, the voltage drop Pn across which is selected by multiple switches S1, S2 to energize one primary of transformer Tr. The voltage Un appearing at each nodal point An is selected by multiple switch S3 ganged with S1, S2 to energize a potentiometer a producing a slider voltage of a Un, and the voltage Un also energizes a potentiometer bn for each nodal point whose slider potential bn Un is selected by multiple switch S4 ganged with S3 to energize a second primary of transformer Tr in. opposition to the voltage a Un so that an error voltage Qn given by equation (4) appears across the secondary for each nodal point of the network selected by the ganged switches in correspondence with different points along the shaft. The series of voltages may be displayed, e.g. on a range of n vibration galvanometers selected in correspondence with the successive outputs of the transformer, or as y-deflections of a long-persistence C.R. oscilloscope wherein the successive Qn traces are shifted along the x axis synchronically with the operation of switches S1 to S4 in selecting successive pairs of network nodal points An, Bn; so that the iterative adjustment of the currents In flowing into each mesh node point so as to reduce Qn to zero in each case is facilitated. Fig. 3 shows a modification in which the several voltages Pn, Un, bn, aUn derived from the successive network sections as shown in Fig. 2, are selected by a 25-way uniselector which is ratchet motor operated from half-wave rectified A.C. to switch at 50 positions per second. Writing E1=Pn, E2= -bn Un, E3= - Un and k2=a0; equation (4) reduces to k2 E3 - E2+E1=Q-(5) which is synthesized by supplying voltages E1 and - E2 from the uniselector contacts to a first subtracting circuit which produces an output voltage - (E1+E2)/(2) and voltage - E3 to a calibrated potentiometer producing an output voltage - kSP2/SPE3/2, which outputs are supplied to a second subtracting circuit to produce an output voltage “(E1+E2 - kSP2/SPE3)= - Q/4. The residual - Q/4 developed for each section of the analogue network and selected by the uniselector is amplified and displayed on a long persistence cathode-ray oscillograph having an x deflection controlled by the same uniselector to increase in successive steps whereby a large number of residuals are displayed together as vertical lines positionally displaced along the x axis in conformity with the positions of the successive nodal points of the network, which lines extend vertically upwards or downwards from the x axis in dependence on the sign of the residual. Spurious voltages arising from switch contact potentials are eliminated by blacking out the C.R. trace for the half-cycle immediately following the instant at which contact is made, so that the spurious voltages are not displayed and the sense of the display represents the sign of each residual error as well as the magnitude. As before, the currents into each network node are iteratively adjusted to reduce each residual voltage to zero for solution of equation (1). The difference circuits may comprise (Fig. 4) a double triode having equal anode resistances and equal cathode bias resistances; the anodes being connected directly to their opposite cathodes by resistances R5, R6. Voltages E1, E2 are applied to respective grids and the difference voltage appears on a sliding tap on resistance R5; adjustable for balance. The resistance analogue network may be D.C. excited, and the uniselector may be operated at such a speed as to act as a chopper; the succeeding amplifier circuits being given an adequate time constant so that the chopped signals are transmitted and are displayed as bright spots positionally displaced with respect to the X-axis of the oscilloscope to give the magnitude and sign of each residual. Specification 684,989 is referred to.
机译:754,113。电气模拟计算设备。联合电气工业有限公司。1953年8月12日[八月1952年1月28日],第21658/52号。类37.一种用于解决代表物理问题的微分方程的电模拟计算设备,其包括电阻网络,该电阻网络以有限差分形式表示该方程的至少一部分,并且具有表示该差分方程的连续位置点的一系列节点结点以及装置。通过将这些电压与满足要解决的问题的所需电压值进行比较,从而将电流馈送到结点并测量其上的合成电压,以便从节点结点导出误差信号,并在视觉阵列中同时显示这些误差信号。可以确定输入调整对各个节点结点处的电压关系的影响。图1示出了电阻器模拟网络的一部分,该电阻器模拟网络用于求解限定旋转轴的临界速度的四阶微分方程,其中x是沿旋转轴的位置。 y是轴的挠度; E是杨氏模量; I是绕轴轴线的转动惯量; m是每单位长度轴的重量; #是临界速度;所述网络包括电阻链N1,N2,所述电阻链N1,N2包括电阻R1,R2并且通过电阻R3互连;电阻R1,R2,R3的值由具有适当比例因子的E,I和m的局部值确定。节点An,Bn代表沿轴轴线测量的一系列位置点中的第n个,将其分为与连续网络网格对应的部分。来自点Cn的电流In通过电阻R4馈入链条N1的点Bn,并且在链条N2的点An处出现了以网络零点为参考测得的电压Un,以表示轴偏转y。 In的值是可调的,并且对于等式(1)的解是可调节的,其中α是比例常数; #x 1 ,#x 11 是x到以An,Bn表示的轴点左右两侧的间隔; #n是在该轴点处的恒定轴承反作用力,因此R4两端的电压降Pn由下式给出:Un,Pn是测得的电压; bn是一个已知常数;对于解决方案中的每个网络网格,ao是# 2 的常数倍;在对解决方案的连续网络迭代调整过程中,Qn是残留误差信号。图2示出了用于系统的网络的迭代调整的设备,在该设备中,针对每个节点的Qn#0和a#ao,其中供应给每个节点Bn的电流In是从交流电源V通过调整可变电阻Rx获得的。串联电阻R4通过多个开关S1,S2选择其上的电压降Pn以激励变压器Tr的一个初级。通过与S1,S2组合的多个开关S3选择出现在每个节点An上的电压Un来给电位器a通电,从而产生一个Un的滑块电压,并且电压Un还为每个节点的滑块电位bn通电一个电位器bn。通过与S3相连的多个开关S4选择Un,以激励变压器Tr in的第二初级,与电压a Un相对,从而对于所选网络的每个节点,由次级方程式(4)给出的误差电压Qn出现在次级上通过联动开关与沿轴的不同点对应。例如,可以显示一系列电压。在与变压器的连续输出相对应的n个振动振镜的范围内选择,或者作为长余辉CR示波器的y偏转选择,其中连续Qn迹线与开关S1至S4的操作沿x轴同步移动在选择连续的网络节点对An,Bn时;因此,便于迭代地调整流入每个网格节点的电流In,从而在每种情况下都将Qn减小为零。图3示出了一种变型,其中由图2所示的连续网络部分得出的几个电压Pn,Un,bn,aUn由25路单选择器选择,该25向单选择器是由半波整流AC操作的棘轮电动机。每秒切换50个位置。写E1 = Pn,E2 = -bn Un,E3 =-Un和k2 = a0;等式(4)简化为k2 E3-E2 + E1 = Q-(5),这是通过从单选择器触点向第一减法电路提供电压E1和-E2产生输出电压-(E1 + E2)/( 2)和电压-E3到校准电位计,产生输出电压-k 2 E3 / 2,其输出被提供给第二减法电路以产生输出电压“(E1 + E2-k 2 E3)=-Q / 4。为模拟网络的每个部分生成并由单选择器选择的残差-Q / 4被放大并显示在长余辉阴极射线示波器上,该示波器具有x偏转,该偏转由同一单选择器控制,从而以连续的步长增加,从而大量残差显示为垂直线,沿着垂直于网络的连续节点的位置沿x轴位置偏移,这些线根据残差的符号从x轴垂直向上或向下延伸。通过在紧接接触后的半周内将CR迹线涂黑,从而消除了由开关接触电势引起的杂散电压,因此不会显示杂散电压,并且显示的感觉代表每个残余的符号误差以及幅度。如前所述,迭代地调整进入每个网络节点的电流以将每个残余电压减小为零,以解决方程式(1)。差分电路可以包括(图4)具有相等的阳极电阻和相等的阴极偏置电阻的双三极管。阳极通过电阻R5,R6直接连接到其相对的阴极。分别将电压E1,E2施加到栅极上,并且差值电压出现在电阻R5的滑动抽头上;可调平衡。电阻模拟网络可以是直流激励的,单选择器可以以斩波器的速度工作;后续的放大器电路具有足够的时间常数,以便斩波后的信号得以传输并显示为相对于示波器X轴位置偏移的亮点,以给出每个残差的大小和正负号。参考规格684989。

著录项

  • 公开/公告号DE000001079865A

    专利类型

  • 公开/公告日1960-04-14

    原文格式PDF

  • 申请/专利权人 SUNVIC CONTROLS LTD;

    申请/专利号DES0035028A

  • 发明设计人 BAILEY ROY;LIEBMANN GERHARD;

    申请日1953-08-28

  • 分类号

  • 国家 DE

  • 入库时间 2022-08-23 19:22:38

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