Superheterodyne seismic vibrator and method
View Patent ↗A seismic energy source includes at least a first and a second acoustic radiator operatively coupled to a non-linear medium proximate an upper limit of formations in the Earth's subsurface. The first and second acoustic radiators are configured to convert electrical energy directly into acoustic energy. The source includes means for operating the first and the second acoustic radiator at respective first and second frequencies. The first and second frequencies are selected such that substantially no acoustic energy propagates through the non-linear medium. The first and the second frequencies are selected such that a difference therebetween is swept through a range of frequencies of seismic energy capable of propagating through the Earth's subsurface to at least one acoustic impedance boundary within the Earth's subsurface.
1. A seismic energy source, comprising:
at least a first and a second acoustic radiator operatively coupled to a non-linear medium proximate an upper limit of formations in the Earth's subsurface, the first and second acoustic radiators configured to convert electrical energy directly into acoustic energy and to have a base or mean operating frequency near or above 10 Khz; and
means for operating the first and the second acoustic radiator at respective first and second frequencies, the first and second frequencies selected near or above 10 Khz and such that substantially no acoustic energy propagates through the non-linear medium, the first and the second frequencies selected such that a difference there between is swept through a range of frequencies of seismic energy capable of propagating through the Earth's subsurface to at least one acoustic impedance boundary within the Earth's subsurface.
2. The source of claim 1 wherein the first and second acoustic radiators comprise piezoelectric devices.
3. The source of claim 1 wherein the first and second acoustic radiators comprise magnetostrictive devices.
4. The source of claim 1 wherein the means for operating is configured to operate the first and second acoustic radiators at about 10 KHz, and a difference between the first and second frequencies is within a range of about zero to 200 Hz.
5. The source of claim 1 further comprising at least one borehole formed through a weathered layer proximate the Earth's surface and filled with a material harder than material of the weathered layer, and wherein the first and second acoustic radiators are placed in contact with the material in the at least one borehole.
6. A method for subsurface surveying, comprising:
operating a first acoustic radiator disposed proximate the upper limit of the Earth's subsurface at a first frequency; and
operating a second acoustic radiator proximate the upper limit of the Earth's subsurface and the first acoustic radiator at a second frequency;
wherein the first and second frequencies are at least about 10 KHz and above a propagation frequency of a non-linear medium proximate the upper limit, and wherein a difference between the first and second frequencies is swept through a range of frequencies capable of propagating seismic energy through the Earth's subsurface to at least one acoustic impedance boundary therein.
7. The method of claim 6 wherein the first and second frequencies are selected such that difference there between is swept through a range of about zero to 200 Hz.
8. The source of claim 1 wherein said range of frequencies is provided by sweeping either or both the first and second frequencies of the first and second acoustic radiators through a range.
9. The source of claim 1 wherein said swept range is the difference of the first frequency being swept through a selected range while the second frequency is swept through the inverse of the selected range.
10. The source of claim 1 wherein the swept range is the difference of the first frequency being held constant while the second frequency is swept through a selected range.
11. The source of claim 9 wherein the first frequency is swept through a range of 9900 to 10100 Hz while the second frequency is swept through the inverse range of 10100 Hz to 9900 Hz, and the superheterodyne frequency is a sweep through a range of 200 Hz to 0 and back to 200 Hz.
12. The source of claim 10 wherein the first frequency is held at a constant 10000 Hz while the second frequency sweeps through a range of 10000 Hz to 10200 Hz, and the superheterodyne frequency sweeps through a range of 0 to 200 Hz.
13. The method of claim 6 wherein the first acoustic radiator and the second acoustic radiator are located in sufficiently close proximity such that the acoustic energy radiates in a substantially spherical pattern.
14. The method of claim 6 wherein the first acoustic radiator and the second acoustic radiator are positioned one with respect to the other such that the acoustic energy radiates in a directed pattern.
15. The method of claim 6 wherein the first and second acoustic radiators are positioned in first and second boreholes, formed through a weathered layer proximate the Earth's surface, that have been filled with a material harder than material of the weathered layer, and wherein the acoustic radiators are placed in contact with said harder material in the boreholes, for transmission of acoustic energy into the Earth's subsurface.
16. The method of claim 15 wherein the acoustic radiators are affixed to the top of the harder material in the boreholes.
17. The method of claim 15 wherein the harder material is concrete.
18. The method of claim 15 wherein the weathered layer is comprised of unconsolidated materials.
19. The method of claim 6 wherein the surveying is on land.
20. The method of claim 6 wherein the surveying is on water or on the water bottom.