The invention provides a method and an apparatus for measuring the size, concentration and size distribution of particles in a fluid by determining the characteristics of an acoustic speckle signal of the particles and relating these characteristics to the size and concentration characteristics of t
The invention provides a method and an apparatus for measuring the size, concentration and size distribution of particles in a fluid by determining the characteristics of an acoustic speckle signal of the particles and relating these characteristics to the size and concentration characteristics of the particles. The method and the apparatus are especially useful for the measurement of the size distribution of small particles in optically opaque liquids.
대표청구항▼
1. A method for determining the size distribution of particles in a fluid comprising the steps of obtaining an acoustic speckle signal of the particles in the fluid and deriving the size distribution of the particles from the acoustic speckle signal. 2. The method as set forth in claim 1, wherein th
1. A method for determining the size distribution of particles in a fluid comprising the steps of obtaining an acoustic speckle signal of the particles in the fluid and deriving the size distribution of the particles from the acoustic speckle signal. 2. The method as set forth in claim 1, wherein the acoustic speckle signal is obtained by introducing an input signal of acoustic energy into the fluid; sensing a portion of scattered acoustic energy resulting from interaction of the particles with the input signal; producing an output signal corresponding to amplitude of the portion of scattered acoustic energy as a function of time; transforming the output signal from a time domain to a frequency domain; and identifying the acoustic speckle signal from the output signal transformed to the frequency domain.3. The method as set forth in claim 2, wherein the input signal is focused on a focal region in the fluid and some of the input signal is scattered by particles in the focal region, and wherein the output signal is limited to the portion of acoustic energy scattered by particles in the focal region.4. The method as set forth in claim 3, wherein the fluid contains particles that produce individual speckle events and wherein the size distribution of the particles in the fluid is derived by calculating, for two or more individual acoustic speckle events, the size of the particles that produced each individual speckle event; measuring the frequency of occurrence of speckle events that were produced by particles having the same size; and deriving the particle size distribution from the frequency of occurrence of speckle events as a function of particle size.5. The method as set forth in claim 4, wherein a sufficient number of particle size calculations are obtained for the calculation of a particle size distribution for the particles in the fluid and wherein the size distribution of particles in the fluid is determined as the frequency of occurrence of acoustic speckle events produced by particles having a certain size.6. The method as set forth in claim 5, comprising at least about 100 particle size calculations.7. The method as set forth in claim 6, comprising at least about 500 particle size calculations.8. The method as set forth in claim 7, comprising at least about 1000 particle size calculations.9. The method as set forth in claim 8, comprising at least about 2000 particle size calculations.10. The method as set forth in claim 4, wherein, for each individual speckle event, the size of the particles that produced that speckle event is derived from the duration of each individual acoustic speckle signal for that individual speckle event by using a diffusion model.11. The method as set forth in claim 10, wherein the diffusion model is of the form:a =(tm)(4kT/6&pgr;η)(8/λerfc(1))2where: a is the particle radius in meters; t mis the duration of an acoustic speckle event in seconds λ is the acoustic wavelength in meters; k is the Boltzman constant (JK −1), (1.38×10−23); T is the absolute temperature in degrees Kelvin; &pgr; is 3.14159; andη is the viscosity of the fluid in Pa·s.12. The method as set forth in claim 4, wherein, for each individual speckle event, the size of the particles that produced that speckle event is derived from the duration of each individual acoustic speckle signal for that individual speckle event by using an autocorrelation model.13. The method as set forth in claim 4, wherein, for each individual speckle event, the size of the particles that produced that speckle event is derived by measuring the amplitude of the acoustic speckle signal that produced that speckle event and correlating the particle size with the maximum amplitude of such acoustic speckle signal.14. The method as set forth in claim 3, where the fluid contains particles that produce individual speckle events and wherein the size distribution of the particles in the fluid is determined from the acoustic speckle signal by, for each of two or more individual speckle events, identifying an individual acoustic speckle signal corresponding to the individual speckle event; measuring the duration of the individual acoustic speckle signal; deriving the size of the particles that produced the individual speckle event from the duration of the individual acoustic speckle signal, determining the volume of the focal region; calculating the concentration of particles having the size of those that produced the individual speckle event from the particle size and the volume of the focal region, and determining the size distribution of particles in the fluid from the particle size and concentration as measured for the two or more speckle events.15. The method as set forth in claim 14, wherein, for each individual speckle event, the size of the particles that produced that speckle event is derived from the duration of the individual acoustic speckle signal for that individual speckle event by using a diffusion model.16. The method as set forth in claim 14, wherein, for each individual speckle event, the size of the particles that produced that speckle event is derived from the duration of the individual acoustic speckle signal for that individual speckle event by using an autocorrelation model.17. The method as set forth in claim 14, wherein, for each individual speckle event, the size of the particles that produced that speckle event is derived by measuring the amplitude of the individual acoustic speckle signal and correlating the particle size with the maximum amplitude of such individual acoustic speckle signal.18. The method as set forth in claim 1, wherein the fluid is a liquid.19. The method as set forth in claim 18, wherein the liquid is a liquid hydrocarbon.20. The method as set forth in claim 19, wherein the liquid hydrocarbon is optically opaque.21. The method as set forth in claim 20, wherein the liquid hydrocarbon is crude oil.22. The method as set forth in claim 18, wherein the input signal of acoustic energy is an input signal of ultrasonic energy.23. The method as set forth in claim 1, wherein the fluid is a liquid hydrocarbon that contains particles that produce individual speckle events by interaction with acoustic energy, and the method comprises the steps of (a) introducing an input signal of acoustic energy into the hydrocarbon, which input signal is focused on a focal region in the hydrocarbon, such that particles in the focal region interact with the input signal to scatter the acoustic energy, producing an output signal of the acoustic energy scattered by the particles in the focal region; (b) sensing the output signal in the form of amplitude as a function of time; (c) transforming the sensed output signal from a time domain to a frequency domain, (d) identifying an acoustic speckle signal from the transformed output signal in the frequency domain; (e) carrying out each of the steps (a), (b), (c) and (d) except on a control liquid that contains no asphaltene particles instead of the hydrocarbon; and (f) determining the size distribution of particles in the hydrocarbon by comparing the acoustic speckle signal derived from the hydrocarbon with the acoustic speckle signal derived from the control liquid.24. The method as set forth in claim 23, wherein the acoustic speckle signal of the hydrocarbon has a magnitude at each of a plurality of frequencies, including a selected frequency, and the acoustic speckle signal of the control liquid has a magnitude at each of the plurality of frequencies, and the comparison of the acoustic speckle derived from the hydrocarbon is compared with the acoustic speckle signal derived from the control liquid by subtracting the magnitude of the acoustic speckle signal of the hydrocarbon liquid at the selected frequency from the magnitude of the acoustic speckle signal of the control liquid at the selected frequency to obtain a difference.25. The method as set forth in claim 23, wherein the sensed outpu t signal is transformed from a time domain to frequency domain by use of a Fast Fourier Transform algorithm.
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