Harry J. Simpson
Research Subjects
Harry J. Simpson has a total of 46 co-authors. Here are the top co-authors by number of shared publications:
- Brian H. Houston
Naval Res. Lab., Code 7130, 4555 Overlook Ave., Washington, DC 20375-5320
14 shared publications - Raymond J. Soukup
U.S. Naval Res. Lab., Acoust. Div., Code 7142, 4555 Overlook Ave. SW, Washington, DC 20375, USA
4 shared publications Alain R. Berdoz
Global Strategies Group (North America) Inc., Largo, MD 20774
3 shared publicationsJoseph A. Bucaro
Excet, Inc., Springfield, VA
3 shared publicationsLarry A. Kraus
Global Strategies Group (North America) Inc., Largo, MD 20774
3 shared publications- Michael D. Collins
Code 7160, Acoustics Division, Naval Research Laboratory, Washington, DC 20375, USA
3 shared publications
Latest Publications
- Open Access
- 1 January 2019
- Published by Acoustical Society of America (ASA) in The Journal of the Acoustical Society of America
- Vol. 145 (1) , EL90-EL96
Demonstration of a quasi-monostatic autonomous underwater vehicle based high duty cycle active sonar
The feasibility of resolving target returns within receive signals collected by a continuously transmitting quasi-monostatic, broadband, autonomous underwater vehicle (AUV) based sonar is explored. Theoretical studies supported by experimental results suggest that it is possible to capture the source-to-receiver coupling response and target scattering with sufficient fidelity during the continuous transmission to enable detection and (potentially) classification processing. Demonstrations focused upon the detection of a bottomed target object at sea using transmit signals with duty cycles of 60% and 100% indicate that such an approach is feasible for a representative AUV-based side looking sonar system operating in shallow water.
- 1 January 2019
- Published by Acoustical Society of America (ASA) in The Journal of the Acoustical Society of America
- Vol. 145 (1) , EL90-EL96
Open AccessDemonstration of a quasi-monostatic autonomous underwater vehicle based high duty cycle active sonar
The feasibility of resolving target returns within receive signals collected by a continuously transmitting quasi-monostatic, broadband, autonomous underwater vehicle (AUV) based sonar is explored. Theoretical studies supported by experimental results suggest that it is possible to capture the source-to-receiver coupling response and target scattering with sufficient fidelity during the continuous transmission to enable detection and (potentially) classification processing. Demonstrations focused upon the detection of a bottomed target object at sea using transmit signals with duty cycles of 60% and 100% indicate that such an approach is feasible for a representative AUV-based side looking sonar system operating in shallow water.
- 1 October 2014
- Published by Acoustical Society of America (ASA) in The Journal of the Acoustical Society of America
- Vol. 136 (4_Suppleme) , 2111
Measurements and modeling of acoustic scattering from targets in littoral environments
- 1 October 2014
- Published by Acoustical Society of America (ASA) in The Journal of the Acoustical Society of America
- Vol. 136 (4_Suppleme) , 2111
Measurements and modeling of acoustic scattering from targets in littoral environments
- 1 November 2011
- Published by Acoustical Society of America (ASA) in The Journal of the Acoustical Society of America
- Vol. 130 (5) , 2681-2686
Experimental testing of the variable rotated elastic parabolic equation
A series of laboratory experiments was conducted to obtain high-quality data for acoustic propagation in shallow water waveguides with sloping elastic bottoms. Accurate modeling of transmission loss in these waveguides can be performed with the variable rotated parabolic equation method. Results from an earlier experiment with a flat or sloped slab of polyvinyl chloride (PVC) demonstrated the necessity of accounting for elasticity in the bottom and the ability of the model to produce benchmark-quality agreement with experimental data [J. M. Collis et al., J. Acoust. Soc. Am. 122, 1987–1993 (2007)]. This paper presents results of a second experiment, using two PVC slabs joined at an angle to create a waveguide with variable bottom slope. Acoustic transmissions over the 100–300 kHz band were received on synthetic horizontal arrays for two source positions. The PVC slabs were oriented to produce three different simulated waveguides: flat bottom followed by downslope, upslope followed by flat bottom, and upslope followed by downslope. Parabolic equation solutions for treating variable slopes are benchmarked against the data.
- 1 November 2011
- Published by Acoustical Society of America (ASA) in The Journal of the Acoustical Society of America
- Vol. 130 (5) , 2681-2686
Experimental testing of the variable rotated elastic parabolic equation
A series of laboratory experiments was conducted to obtain high-quality data for acoustic propagation in shallow water waveguides with sloping elastic bottoms. Accurate modeling of transmission loss in these waveguides can be performed with the variable rotated parabolic equation method. Results from an earlier experiment with a flat or sloped slab of polyvinyl chloride (PVC) demonstrated the necessity of accounting for elasticity in the bottom and the ability of the model to produce benchmark-quality agreement with experimental data [J. M. Collis et al., J. Acoust. Soc. Am. 122, 1987–1993 (2007)]. This paper presents results of a second experiment, using two PVC slabs joined at an angle to create a waveguide with variable bottom slope. Acoustic transmissions over the 100–300 kHz band were received on synthetic horizontal arrays for two source positions. The PVC slabs were oriented to produce three different simulated waveguides: flat bottom followed by downslope, upslope followed by flat bottom, and upslope followed by downslope. Parabolic equation solutions for treating variable slopes are benchmarked against the data.
- 1 October 2011
- Published by Acoustical Society of America (ASA) in The Journal of the Acoustical Society of America
- Vol. 130 (4_Suppleme) , 2341
Acoustic imaging and structural acoustic analysis of laboratory measurements of scattering from buried targets above critical grazing angles
- 1 October 2011
- Published by Acoustical Society of America (ASA) in The Journal of the Acoustical Society of America
- Vol. 130 (4_Suppleme) , 2341
Acoustic imaging and structural acoustic analysis of laboratory measurements of scattering from buried targets above critical grazing angles
- 1 October 2009
- Published by Acoustical Society of America (ASA) in The Journal of the Acoustical Society of America
- Vol. 126 (4_Suppleme) , 2167
Scattering by unexploded ordnance with variable burial depth and seafloor roughness: A parametric study.
- 1 October 2009
- Published by Acoustical Society of America (ASA) in The Journal of the Acoustical Society of America
- Vol. 126 (4_Suppleme) , 2167
Scattering by unexploded ordnance with variable burial depth and seafloor roughness: A parametric study.
- 1 April 2009
- Published by Acoustical Society of America (ASA) in The Journal of the Acoustical Society of America
- Vol. 125 (4_Suppleme) , 2733
The broadband in-water structural acoustics of unexploded ordinance: Tank comparisons with at-sea rail measurements.
- 1 April 2009
- Published by Acoustical Society of America (ASA) in The Journal of the Acoustical Society of America
- Vol. 125 (4_Suppleme) , 2733
The broadband in-water structural acoustics of unexploded ordinance: Tank comparisons with at-sea rail measurements.
- 1 April 2009
- Published by Acoustical Society of America (ASA) in The Journal of the Acoustical Society of America
- Vol. 125 (4_Suppleme) , 2734
Long-range low frequency shallow water acoustic propagation and bottom penetration experiments for underwater unexploded ordinance.
- 1 April 2009
- Published by Acoustical Society of America (ASA) in The Journal of the Acoustical Society of America
- Vol. 125 (4_Suppleme) , 2734
Long-range low frequency shallow water acoustic propagation and bottom penetration experiments for underwater unexploded ordinance.
- 1 May 2008
- Published by Acoustical Society of America (ASA) in The Journal of the Acoustical Society of America
- Vol. 123 (5_Suppleme) , 3602
The Broadband In-Water Structural Acoustics of Unexploded Ordinance
The Laboratory for Structural Acoustics (LSA) at the Naval Research Laboratory consists of a 1 million gallon, deionized water, indoor cylindrical tank (17m diameter by 15m deep). The key features include: 1) vibration and temperature isolation, 2) feedback controlled heating and adiabatic materials (temperature variability <0.01°C), and 3) reverberation reducing anechoic materials. This laboratory has computer controlled roboticscanners and manipulators used for precision freefield measurements including nearfield acoustic holography and compact range scattering. The precision robotics, environmental control, and painstaking measures to insure homogeneity and stability result in a high fidelity, versatile, and unique underwater acousticmeasurement laboratory. The LSA also contains an indoor rectangular tank (10m by 8m) laboratory, with a 3m deep sand bottom and 4m of water column. In a similar fashion to the freefield laboratory, this laboratory is used to study target scattering in a marine bottom environment. We discuss such databases focused on the challenging problem of unexploded ordinance (UXO) in water where we use the structural acoustic response measured in a series of laboratory experiments to detect and identify several common UXOs. The 360 degree broadband (1‐140 kHz) compact range monostatic and bistatic measurements taken in both laboratories will be discussed.
- 1 May 2008
- Published by Acoustical Society of America (ASA) in The Journal of the Acoustical Society of America
- Vol. 123 (5_Suppleme) , 3602
The Broadband In-Water Structural Acoustics of Unexploded Ordinance
The Laboratory for Structural Acoustics (LSA) at the Naval Research Laboratory consists of a 1 million gallon, deionized water, indoor cylindrical tank (17m diameter by 15m deep). The key features include: 1) vibration and temperature isolation, 2) feedback controlled heating and adiabatic materials (temperature variability <0.01°C), and 3) reverberation reducing anechoic materials. This laboratory has computer controlled roboticscanners and manipulators used for precision freefield measurements including nearfield acoustic holography and compact range scattering. The precision robotics, environmental control, and painstaking measures to insure homogeneity and stability result in a high fidelity, versatile, and unique underwater acousticmeasurement laboratory. The LSA also contains an indoor rectangular tank (10m by 8m) laboratory, with a 3m deep sand bottom and 4m of water column. In a similar fashion to the freefield laboratory, this laboratory is used to study target scattering in a marine bottom environment. We discuss such databases focused on the challenging problem of unexploded ordinance (UXO) in water where we use the structural acoustic response measured in a series of laboratory experiments to detect and identify several common UXOs. The 360 degree broadband (1‐140 kHz) compact range monostatic and bistatic measurements taken in both laboratories will be discussed.
- 1 May 2008
- Published by Acoustical Society of America (ASA) in The Journal of the Acoustical Society of America
- Vol. 123 (5_Suppleme) , 3602
Shallow-water tank experiments and model comparisons over range-dependent elastic bottoms
A series of tank experiments has been conducted in order to obtain high quality data for acoustic propagation in shallow‐water environments with elastic bottoms. Such problems can now be solved accurately with the parabolic equation method, which is being used for comparisons with measured transmission loss. Results from the initial experiment with a flat or sloped slab of PVC demonstrated both benchmark quality agreement between computed solutions and data, and the necessity of accounting for elasticity in the bottom [J. M. Collis, et al., JASA 122]. This paper will present results of a second experiment, conducted in the same manner as the first, but modified to allow for variable bottom slopes. Time series were collected at 100‐300 kHz on horizontal arrays for two source positions. Parabolic equation solutions for treating variable slopes, using coordinate transformation methods of mapping and axis rotations, will be benchmarked against the new data. [Work supported by the Office of Naval Research.]
- 1 May 2008
- Published by Acoustical Society of America (ASA) in The Journal of the Acoustical Society of America
- Vol. 123 (5_Suppleme) , 3602
Shallow-water tank experiments and model comparisons over range-dependent elastic bottoms
A series of tank experiments has been conducted in order to obtain high quality data for acoustic propagation in shallow‐water environments with elastic bottoms. Such problems can now be solved accurately with the parabolic equation method, which is being used for comparisons with measured transmission loss. Results from the initial experiment with a flat or sloped slab of PVC demonstrated both benchmark quality agreement between computed solutions and data, and the necessity of accounting for elasticity in the bottom [J. M. Collis, et al., JASA 122]. This paper will present results of a second experiment, conducted in the same manner as the first, but modified to allow for variable bottom slopes. Time series were collected at 100‐300 kHz on horizontal arrays for two source positions. Parabolic equation solutions for treating variable slopes, using coordinate transformation methods of mapping and axis rotations, will be benchmarked against the new data. [Work supported by the Office of Naval Research.]
- 1 May 2008
- Published by Acoustical Society of America (ASA) in The Journal of the Acoustical Society of America
- Vol. 123 (5_Suppleme) , 3601
Backscattering From Scale Models of Elastic Ocean Bottoms with Power-law Roughness
Rough surface analogs to ocean bottom interfaces with two contrasting power-law roughness spectra were fabricated from slabs of PVC. A tank experiment with a nearly monostatic geometry and transmitted signals in the band 100-300 kHz was performed, with the source and receiver positioned to produce acoustic interactions on multiple locations on the surfaces. Models of scattering strength and the received time series, using deterministic and stochastic representations of the surface, are used to verify the predicted dependence of the scattering, with emphasis on the sub-critical angle (< 50 degrees grazing) region, where the predicted difference in scattering strength due to the contrast in roughness between the two fabricated surfaces is on the order of 10 dB. The numerical models employed were perturbation theory, a second-order small-slope calculation using the power-law roughness parameters, and a fourth-order small-slope calculation using the actual grid of heights as an input. The experimental effort also focused on the near-critical angle region where the predictions of the numerical models differed markedly. [Work supported by ONR and NURC.]
- 1 May 2008
- Published by Acoustical Society of America (ASA) in The Journal of the Acoustical Society of America
- Vol. 123 (5_Suppleme) , 3601
Backscattering From Scale Models of Elastic Ocean Bottoms with Power-law Roughness
Rough surface analogs to ocean bottom interfaces with two contrasting power-law roughness spectra were fabricated from slabs of PVC. A tank experiment with a nearly monostatic geometry and transmitted signals in the band 100-300 kHz was performed, with the source and receiver positioned to produce acoustic interactions on multiple locations on the surfaces. Models of scattering strength and the received time series, using deterministic and stochastic representations of the surface, are used to verify the predicted dependence of the scattering, with emphasis on the sub-critical angle (< 50 degrees grazing) region, where the predicted difference in scattering strength due to the contrast in roughness between the two fabricated surfaces is on the order of 10 dB. The numerical models employed were perturbation theory, a second-order small-slope calculation using the power-law roughness parameters, and a fourth-order small-slope calculation using the actual grid of heights as an input. The experimental effort also focused on the near-critical angle region where the predictions of the numerical models differed markedly. [Work supported by ONR and NURC.]