【发明专利】 Improvements in or relating to apparatus for dividing high frequency power
显示摘要
592,161. Coil -- less resonators. SPERRY GYROSCOPE CO., Inc. July 23, 1943, No. 24309/45. Convention date, Feb. 4, 1942. Divided out of 592,119. [Class 40 (iii)] [Also in Group XXXVI] Apparatus having broad frequency band characteristics is arranged so as to, effect energy division in a concentric line. As shown in Fig. 1, two hollow end conductors 25, 26 are held a fixed distance apart by a member 27 and terminated by tapered concentric line adaptors 28, 28<1> adapted to receive concentric transmission line terminals. A central member 29 is slidably mounted between the two end members 25, 26 and can be fixed in adjusted position by a screw 30 slidable in a slot in the member 27. The inner conductor of the central member 29 has a varying diameter, whilst the outer conductor is of constant diameter. The central member 29 is provided with a high impedance tap 34 at its lowest impedance point, where the inner conductor has a sudden reduction in diameter, corresponding to an increase in impedance. The tap 34 has attached to it an outer conductor 54 of constant inner diameter and an inner conductor 53 of slowly increasing diameter, so that at the point 55 the impedance of the line is equal to that of the line to be attached. In order to allow for the effect of standing waves due to energy reflections, the position of the tap between the two fixed end sections 25, 26 is varied so as to obtain maximum and minimum readings from which the actual energy transfer along the transmission line may be determined. In order to minimize end reflections due to wall thickness at a sliding joint in a concentric line, the tube end may be cut at an angle as shown at 32, Fig. 2, or may be terminated in a helix 32<1>, Fig. 3. Alternatively, the ends of the sliding tubes exposed to the travelling waves may be staggered by a distance equal to a quarter wavelength as described in Specification 581,972. In the alternative form of current or energy dividing device shown in Fig. 4, energy to be divided is introduced into the tapered matching end 59 and is divided into calculable portions at the tap 341. The portion tapped by the branch 49<1> is fed to a device for measurement or other purposes whilst the remainder travels into a terminating impedance 36, which may be of carbon, graphite, or other semi-conductor. The unused energy is entirely absorbed and no reflection can occur to cause a standing wave at the tap 34<1>, which may therefore be fixed. In a modification, Fig. 5, the inner conductor is stepped at 62, 63, 64, 65, 67, 68, 69 and the inner conductor of the branch is stepped at 66, 67, 72, 73. The steps are such that the change in the logarithm of the impedance at each step is proportional to the corresponding binomial coefficient of order one less than the number of steps. Two or more of the current dividing devices shown in Figs. 1, 4 or 5 may be used in cascade. The outer conductor may vary in diameter.