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High frequency impedance measuring apparatus using two bidirectional couplers

  • US 4,780,661 A
  • Filed: 07/31/1986
  • Issued: 10/25/1988
  • Est. Priority Date: 08/02/1985
  • Status: Expired due to Fees
First Claim
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1. In a high frequency impedance measurement apparatus:

  • a first bidirectional coupler is inserted, by means of line sections having a known characteristic impedance Zc, between a generator generating a high frequency wave of variable power and electrodes between which is placed a body whose impedance Z, unknown, is to be measured,the first coupled channel of said first coupler measuring the incident wave on the impedance Z, is connected through a second bidirectional coupler and a single inverter, to an impedance of one of the following types;

    a zero impedance, a practically infinite impedance, and a first matched load,the second coupled channel of said first coupler measuring the wave reflected by the impedance Z, is connected through a first inverter of a double inverter, either to a second matched load or, through a first variable attenuator, to the input of a first power divider without phase shift between its two outputs connected to the RF inputs of two mixers,the first coupled channel of said second coupler measuring the incident wave towards said single inverter, is connected through a second variable attenuator to the input of a second power divider with a phase shift of 90 degrees between its two outputs connected to the LO input of said two mixers,the second coupled channel of said second coupler measuring the wave reflected from said single inverter being connected through the second inverter of said double inverter, either to the input of said first attenuator when said second coupled channel of said first coupler is connected to said second matched load, or to a third matched load when said second coupled channel of said first coupler is connected to the input of said first attenuator,the IF output of said two mixers delivering two signals representing the real part and the imaginary part, respectively, of the value of the incident wave on the impedance Z when said single and double inverters are in their first positions, and the real part and the imaginary part of the value of the wave reflected by the impedance Z when said single and double inverters are in their second position, from which may be determined the coefficient of reflection of impedance Z, then impedance Z by the relationship
    
    
    space="preserve" listing-type="equation">Z=Zc(1+ρ

    )/(1-ρ

    ).

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