Fluid density from tunable acoustic impedance matching
Downhole tools for measuring properties of a fluid include a sample chamber configured to receive the fluid, a field responsive material (“FRM”) arranged with an interface between the field responsive material and the fluid under test in the sample chamber. The field responsive material is tunable to change an acoustic impedance of the field responsive material in response to application of an applied field. A field generator is arranged in relation to the field responsive material, the field generator configured to generate and apply a field to the field responsive material. An acoustic transducer is arranged to direct acoustic energy into and through the field responsive material toward the interface between the field responsive material and the fluid and configured to detect reflections of acoustic energy that reflect from the interface.
1. A downhole tool for measuring properties of a fluid, the downhole tool comprising:
a sample chamber configured to receive the fluid;
a field responsive material arranged with an interface between the field responsive material and the fluid in the sample chamber, wherein the field responsive material is tunable to change an acoustic impedance of the field responsive material in response to application of an applied field;
a field generator arranged in relation to the field responsive material, the field generator configured to generate and apply a field to the field responsive material; and
an acoustic transducer arranged to direct acoustic energy into and through the field responsive material toward the interface between the field responsive material and the fluid and configured to detect reflections of acoustic energy that reflect from the interface.
2. The downhole tool of claim 1 , further comprising:
a controller in operable communication with the field generator, the controller configured to cause generation of different strength fields from the field generator.
3. The downhole tool of claim 2 , wherein the controller is configured to perform a sweep operation to change the field strength to determine a minimum reflection of acoustic energy from the interface.
4. The downhole tool of claim 1 , wherein the field responsive material is a magnetorheological material.
5. The downhole tool of claim 4 , wherein the field generator is configured to generate a magnetic field that is applied to the magnetorheological material to change an acoustic impedance thereof.
6. The downhole tool of claim 1 , wherein the field responsive material is an electrorheological material.
7. The downhole tool of claim 6 , wherein the field generator is configured to generate an electric field that is applied to the electrorheological material to change an acoustic impedance thereof.
8. The downhole tool of claim 1 , further comprising:
a fluid interface member arranged at the interface between the field responsive material and the fluid in the sample chamber.
9. The downhole tool of claim 1 , further comprising:
a transducer interface member arranged at an interface between the acoustic transducer and the field responsive material.
10. The downhole tool of claim 1 , further comprising:
a sampling probe member arranged to extract a fluid from a downhole formation and direct said extracted fluid to the fluid sample chamber.
11. A method for determining fluid properties with a downhole tool having a sample chamber, a field responsive material, an acoustic transducer, and a field generator, the method comprising:
filling the sample chamber with a fluid;
applying a field to the field responsive material, using the field generator, to cause an acoustic impedance of the field responsive material to change to a predetermined acoustic impedance;
directing acoustic energy through the field responsive material, from the acoustic transducer to an interface between the field responsive material and the fluid in the sample chamber;
monitoring acoustic energy reflections from the interface to determine an acoustic impedance of the fluid in the sample chamber;
changing the applied field to alter the acoustic impedance of the field responsive material;
determining an acoustic impedance of the field responsive material that has a minimum amount of acoustic energy reflection; and
obtaining an acoustic impedance of the fluid in the sample chamber from the determined acoustic impedance of the field responsive material.
12. The method of claim 11 , wherein the field responsive material is a magnetorheological material.
13. The method of claim 12 , wherein the field generator is configured to generate a magnetic field that is applied to the magnetorheological material to change an acoustic impedance thereof.
14. The method of claim 11 , wherein the field responsive material is an electrorheological material.
15. The method of claim 14 , wherein the field generator is configured to generate an electric field that is applied to the electrorheological material to change an acoustic impedance thereof.
16. The method of claim 11 , wherein the steps of applying a field, directing acoustic energy, and monitoring acoustic energy reflections is performed in a stepwise manner with the changing of the applied field to find a minimum reflection of the acoustic energy.
17. The method of claim 11 , further comprising:
measuring a sound speed of the fluid using a sound speed sensor tool; and
calculating a fluid mass density from the measured sound speed and the obtained acoustic impedance of the fluid in the sample chamber.
18. The method of claim 11 , further comprising:
obtaining acoustic reflection information during monitoring of the acoustic energy reflections;
applying a best fit polynomial to the acoustic reflection information; and
obtaining a first derivative of the best fit polynomial and determining where said first derivative crosses zero to obtain the fluid acoustic impedance of the fluid in the sample chamber.
19. The method of claim 11 , wherein the applied field is selected to achieve an acoustic impedance of the field responsive material between 0.8 Mrayls and 1.8 Mrayls.
20. The method of claim 11 , wherein the acoustic impedance of the fluid in the sample chamber is equal to the acoustic impedance of the field responsive material when the acoustic energy reflections are at a minimum.