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Improvements in and relating to electrical variable impedance device
Improvements in and relating to electrical variable impedance device
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机译:电气可变阻抗设备及其相关的改进
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855,907. Magnetic amplifiers. ENGLISH ELECTRIC CO. Ltd. July 17, 1957 [April 18, 1956], No. 11836/56. Class 40 (9). [Also in Groups XXXV and XL (c)] A cross-field variable inductor comprises a magnetic core having a part 10a which is subjected to a saturating field due to a polarizing winding 12 which is crossed by a field due to an A.C. winding 11, the currents through the windings being proportional. In a certain range of saturation the inductance L of the A.C. winding is inversely proportional to the polarizing current so that the device may be used in a voltage stabilizer (Fig. 8). In that Figure an A.C. winding 52 is connected in series with a polarizing winding 51 fed through a full-wave rectifier 53 and filter 54. Since the current i through winding 52 is the polarizing current and the inductance of winding 52 is inversely proportional to this current, the product Li is constant and hence the voltage across winding 52 is constant at constant frequency. The Provisional Specification also discloses an automatic tuning control (Fig. 9) and a frequency doubling circuit (Fig. 10). In Fig. 9 in order that the circuit 62, 63 should resonate for any of a range of frequencies the inductance of winding 62 must be given by L = K/wSP2/SP where w is the frequency and hence I the polarizing current must be proportional to wSP2/SP, i.e. proportional to 2ww 0 -w 0 SP2/SP where w 0 is a fixed frequency in the range. Hence a first polarizing winding 61a is fed from a voltage source E with a voltage pSP2/SPE corresponding with a current proportional to w 0 SP2/SP and a winding 61b is oppositely fed with a voltage dependent on the frequency w derived from a resistor 65 through a device 67 as in Fig. 8 above, and on pE so as to correspond with 2ww 0 . The factor p is determined by sliders of three ganged potentiometers such that a different p provides a different w 0 . Fig. 10 discloses a frequency doubling circuit in which the variable inductance winding 72 is in series with a resistor 73 and is fed from a source E sin wt. Two polarizing windings are provided carrying currents I o and I 0 sin wt. Since L α K/I the current through the winding 72 comprises two components one of frequency w and the other of frequency 2w, the former being filtered out by a capacitance 74 and the output voltage being obtained across resistor 73. Various constructional forms of the impedance device are disclosed in the Provisional Specification also. Specification 841,866 is referred to.
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机译:855,907。磁放大器。 1957年7月17日[1956年4月18日],编号11836/56。 40级(9)。 [也在XXXV和XL(c)组中]跨场可变电感器包括磁芯,该磁芯具有部分10a,该部分由于极化绕组12而受到饱和场的作用,该极化场被由于交流绕组11引起的场所交叉。 ,流经绕组的电流成比例。在一定的饱和范围内,交流绕组的电感L与极化电流成反比,因此该器件可用于稳压器中(图8)。在该图中,交流绕组52与通过全波整流器53和滤波器54馈入的极化绕组51串联。由于流经绕组52的电流i是极化电流,绕组52的电感与此成反比在电流中,乘积Li是恒定的,因此绕组52两端的电压在恒定频率下是恒定的。该临时规范还公开了一种自动调谐控制(图9)和一个倍频电路(图10)。在图9中,为了使电路62、63在任何频率范围内谐振,绕组62的电感必须由L = K / w 2 SP>给出,其中w是频率,因此I极化电流必须与w 2 SP>成正比,即与2ww 0 -w 0 2 SP>成正比,其中w 0是该范围内的固定频率。因此,从电压源E向第一极化绕组61a馈送电压p 2 SP> E,该电压对应于与w 0 2 SP>成比例的电流,并且向绕组61b反向馈电。电压取决于从电阻器65通过上面的图8中的装置67导出的频率w,并且取决于pE,以对应于2ww 0。因子p由三个组合电位器的滑块确定,以便不同的p提供不同的w 0。图10公开了一种倍频电路,其中可变电感绕组72与电阻器73串联并且从源E sin wt馈电。提供两个极化绕组,其承载电流I o和I 0 sin wt。由于LαK / I,流经绕组72的电流包括两个成分,一个成分为频率w,另一个成分为频率2w,前者被电容74滤除,并且在电阻器73两端获得输出电压。临时规范中也公开了阻抗设备。参考规范841,866。
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