Amplitude and phase detector in a harmonic oscillator system

• US 4,378,698 A
• Filed: 05/01/1981
• Issued: 04/05/1983
• Est. Priority Date: 05/01/1981
• Status: Expired due to Fees

• Current Assignee: Mobil Oil Corporation (Exxon Mobil Corporation)
• Original Assignee: Mobil Oil Corporation (Exxon Mobil Corporation)
• Inventors: Sexton, James H., Medlin, William L., Masse, Lucien
• Primary Examiner(s): Birmiel, Howard A.
• Application Number:
  US06/259,770
• Time in Patent Office: 704 Days
• Field of Search: 73/579, 73/581, 73/594, 73/662, 73/668, 73/778
• US Class Current: 73/579
• CPC Class Codes: G01N 3/38 generated by electromagnetic means
• CPC Class Codes: G01N 33/241 for hydrocarbon content

Abstract

A harmonic oscillator and motion detection system for use in measuring dynamic elastic constants of rock material samples includes a pair of masses vertically suspended from a support position by a pair of wires. At least one mass is driven by a permanent magnet with the driving coil positioned in the air gap to the magnet. The rock sample is horizontally positioned between the pair of masses such that the rock sample acts as a spring element connecting the masses, thereby forming the simple harmonic oscillator. The motion detection system includes a pair of coil-magnets mounted to each mass for use in determining the amplitude and phase of the motion of the pair of masses.

Claims

1. In a system for measuring dynamic elastic constants of rock materials having a rock material horizontally supported between a pair of masses which are vertically suspended and a coil-magnet system driven by a sinusoidal current such that the masses move in opposition with the rock material acting as a spring element connecting them, the improvement comprising:

(a) a pair of coil-magnet displacement detectors mounted on each of said masses,

(b) means for connecting the coils of said coil-magnet displacement detectors so as to produce an emf displacement signal across said coils that is proportional to the relative displacements of said masses,

(c) a resistive element connected in series with the driving coils to said masses, whereby the voltage across said resistive element has the same phase as said sinusoidal driving current,

(d) means for utilizing the voltage across said resistive element to produce a first square wave signal in phase with the driving current and a second square wave signal 90°

out of phase with said first square wave signal,

(e) a synchronous detector to which said displacement signal and said first square wave signal are applied, said detector producing a output when said displacement signal is in phase with said first square wave signal,

(f) a quadrature detector to which said displacement signal and said second square wave signal are applied, said detector producing a signal when said displacement signal is in phase with said second square wave signal.

2. The system of claim 1 further including means for converting the signals from said synchronous and quadrature detectors into a representation of the amplitude and phase motion of said masses.

3. The system of claim 1 wherein a first of said displacement detectors on each of said masses are located such that they move towards one another as the masses rotate about their vertical support and the second of said displacement detectors on each of said masses are located such that they move away from one another as the masses rotate about their vertical support.

4. The system of claim 3 wherein the magnet coils of said displacement detectors are connected in series such that the emf'"'"'s of the pair of magnet coils located on one of said masses are in polarity opposition to the emf'"'"'s of the pair of magnet coils located on the other of said masses.