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    • 52. 发明专利
    • AT176563T
    • 1999-02-15
    • AT94916840
    • 1994-05-30
    • MARTIN COMMUNICATIONS PTY LTD
    • BEARD DAVID LEWISMARTIN ANDREW LOUIS
    • G01R31/28H04B1/10H04B17/00H04B17/391H04L12/26
    • PCT No. PCT/AU94/00287 Sec. 371 Date Dec. 5, 1995 Sec. 102(e) Date Dec. 5, 1995 PCT Filed May 30, 1994 PCT Pub. No. WO94/29975 PCT Pub. Date Dec. 22, 1994A fading simulator for generating multipath-faded test signals which have attenuation notches of precisely controllable frequency position and attenuation depth from a modulated input signal of known bandwidth. The input signal is fed to a splitter that directs two in-phase components to a first path and a second path. The input to each path is divided by a splitter into in-phase and quadrature sub-signals having a quadrature phase relationship, each sub-signal being fed to a respective inverting attenuator, the outputs of the attenuators then being combined in a combiner and the combined output being passed through a variable delay line to generate the output of the respective path. The outputs of each path are then combined in a combiner circuit to generate the multipath-faded test signal. All four inverting attenuators are preferably substantially identical to one another so that the two paths have close to identical temperature-drift and other characteristics. The attenuators and delay lines are electronically controlled in tandem, preferably using a microprocessor and stored program, to generate precision, static or dynamic, attenuation notches desired.
    • 55. 发明专利
    • Method for laboratory simulation of multipath fading processes
    • DE3619175A1
    • 1987-12-10
    • DE3619175
    • 1986-06-06
    • ANT NACHRICHTENTECH
    • BESSAI HORST DR INGLOREK WERNER DR ING
    • G01R27/28G01R29/00H04B17/391H04B17/00
    • To simulate multi-path fading processes on microwave links in the laboratory, a frequency-selective variable attenuation is to be achieved in the transmission band. For this purpose, the transmitted signal x is split in familiar manner into a direct and an indirect beam which, before they are recombined, are subject to different attenuation and propagation-time influences. The indirect beam is produced after passing through a lambda /4 resonator, the terminating impedance and resonator length l of which can be changed. Recombination with the direct beam is carried out by heterodyning the latter with the echo signal returning from the lambda /4 resonator due to a mismatch, the depth of the attenuation dip being determined by the terminating impedance, its frequency deviation from the centre frequency of the transmission band being determined by the resonator length l. By connecting a number of lambda /4 resonators, decoupled by isolating amplifiers, in cascade, a number of frequency-selective attenuation dips can be achieved. If the length of the lambda /4 resonator is changed by adding or disconnecting discrete line sections via a computer-controlled (9) switching matrix (16) and if its resistive termination is changed via a voltage-controlled field-effect transistor (17), an automatic signature measurement is possible (Figure 3).