Patent GB-736602-A (GB)
Title: Improvements in or relating to frequency spectrum analysers
Inventor: WRIGHT PETER MAURICE
IPC: G01S13/34
Filed: 1952-10-24
Abstract: 736,602. Frequency measurement. MARCONI'S WIRELESS TELEGRAPH CO., Ltd., and BUCKINGHAM, J. Aug. 13, 1953 [Oct. 24, 1952], No. 26808/52. Class 37. [Also in Group XL (c)] A frequency spectrum analyser particularly adapted for displaying received signals of frequency modulated radar systems comprises a mixer wherein incoming signals within the band to be analysed are combined with local signals from a frequency modulated sweep oscillator of deviation approximately equal to the input band width and a dispersive network supplied with a mixer output and adapted to convert the resulting frequency modulated signal trains into signal pulses occurring at times dependent, with respect to the occurrence of the trains at the network input, on the positions of the respective signal frequencies in the input pass band. In Fig. 1, a band of frequencies fa-fb to be analysed is selected by a band-pass filter 1 and applied to a mixer 2 together with the output of a sweep oscillator 3 frequency modulated by a sawtooth law over a band f1-f2 having the same deviation frequency S as the input band, at a repetition frequency fr determined by the x time base of a cathode-ray tube 6. The difference (or sum) frequency band is selected by a filter 7 feeding a delay line 8 having tappings respectively connected to plural narrow band-pass filters F1-FN, each of pass-band and mid-frequency separation fr, covering a band extending from f2-fa to f1-fb. The outputs are combined in a common rectifier 9 energizing the Y plates of the C.R. tube, which displays pulses displaced along the x axis in accordance with their positions in the input frequency band. It is shown that the delay time T of the line over the band of input frequencies applicable thereto must be such that where #f is the required resolution and f is the instantaneous frequency of the sweep oscillator, and for a given oscillator frequency fs the time interval Ta between the appearance of signals of frequency fa-fs and fb-fs is given by while the member N of resolvable points is given by fa-fb/#f. If the filter 7 and the dispersive network are given pass-bands sufficient to admit both sum and difference frequencies, two trains of pulses which are respectively mirror images of each other in time will be produced, and may be displayed as a spectrum by providing an x display time-base operating in opposite senses for each train, with a suitable time interval between the deflections for coincidence of the pulses of the respective trains. Each filter may be succeeded (Fig. 2, not shown) or preceded (Fig. 3, not shown) by a separate delay line, while the several filters may be fed in parallel from the output of filter 7 and inject their respective outputs into appropriate tappings of a delay line (Fig. 4, not shown) supplying rectifier 9. Fig. 5 shows in detail the dispersive network of Fig. 1 wherein the delay line comprises plural sections each composed of mutually coupled series inductances shunted by capacitances C2 and shunted to earth from the inductance junction points by capacitances C1 ; the whole being terminated in its characteristic impedance Rz. The junctions between successive sections supply tuned anode filter-amplifiers F1-Fn resonating at the required frequencies and coupled to the grid of a rectifier amplifier ON by capacitances CC 1-CCN sufficiently small to reduce cross-coupling between the line sections. Adjacent filters may be separated by pairs of bridged T delay sections, and coupling valves may be inserted between the several filter outputs and the common output line. An improved form of display pulse is obtained by amplitude modulating the sweep oscillator signal in accordance with a cosine law and doubling the deviation appropriate to a constant amplitude signal. The frequency band to be analysed may be derived (Fig. 11, not shown) from radar system in which a transmitter radiates a signal which is frequency modulated in accordance with a sawtooth law in synchronism with the x time base of the C.R. tube to produce received signals which are mixed with signals derived directly from the transmitter to produce the frequency band for analysis, which is again mixed with a sawtooth sweep oscillation synchronized with the transmitter repetition frequency to produce further signals exciting the dispersive network whose filters have a bandwidth sufficient to accommodate the Doppler frequency variations due to target motion. Fixed targets are displaced as identical signal pulses centred at the transmitter repetition frequency, and target motion shifts these pulses over the display. The device is stated to be applicable to a P.P.I. display. Specification 647,583, [Group XL (c)], is referred to.