Acoustic and cavitation fields of shock wave therapy devices
Extracorporeal shock wave therapy (ESWT) is considered a viable treatment modality for orthopedic ailments. Despite increasing clinical use, the mechanisms by which ESWT devices generate a therapeutic effect are not yet understood. The mechanistic differences in various devices and their efficacies...
| Main Authors: | , |
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| Format: | Journal article |
| Language: | English |
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2006
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| _version_ | 1826271794448826368 |
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| author | Chitnis, P Cleveland, R |
| author_facet | Chitnis, P Cleveland, R |
| author_sort | Chitnis, P |
| collection | OXFORD |
| description | Extracorporeal shock wave therapy (ESWT) is considered a viable treatment modality for orthopedic ailments. Despite increasing clinical use, the mechanisms by which ESWT devices generate a therapeutic effect are not yet understood. The mechanistic differences in various devices and their efficacies might be dependent on their acoustic and cavitation outputs. We report acoustic and cavitation measurements of a number of different shock wave therapy devices. Two devices were electrohydraulic: one had a large reflector (HMT Ossatron) and the other was a hand-held source (HMT Evotron); the other device was a pneumatically driven device (EMS Swiss DolorClast Vet). Acoustic measurements were made using a fiber-optic probe hydrophone and a PVDF hydrophone. A dual passive cavitation detection system was used to monitor cavitation activity. Qualitative differences between these devices were also highlighted using a high-speed camera. We found that the Ossatron generated focused shock waves with a peak positive pressure around 40 MPa. The Evotron produced peak positive pressure around 20 MPa, however, its acoustic output appeared to be independent of the power setting of the device. The peak positive pressure from the DolorClast was about 5 MPa without a clear shock front. The DolorClast did not generate a focused acoustic field. Shadowgraph images show that the wave propagating from the DolorClast is planar and not focused in the vicinity of the hand-piece. All three devices produced measurable cavitation with a characteristic time (cavitation inception to bubble collapse) that varied between 95 and 209 μs for the Ossatron, between 59 and 283 μs for the Evotron, and between 195 and 431 μs for the DolorClast. The high-speed camera images show that the cavitation activity for the DolorClast is primarily restricted to the contact surface of the hand-piece. These data indicate that the devices studied here vary in acoustic and cavitation output, which may imply that the mechanisms by which they generate therapeutic effects are different. © 2006 American Institute of Physics. |
| first_indexed | 2024-03-06T22:02:20Z |
| format | Journal article |
| id | oxford-uuid:4f04159c-e0d0-4400-821c-899198421faf |
| institution | University of Oxford |
| language | English |
| last_indexed | 2024-03-06T22:02:20Z |
| publishDate | 2006 |
| record_format | dspace |
| spelling | oxford-uuid:4f04159c-e0d0-4400-821c-899198421faf2022-03-26T16:04:38ZAcoustic and cavitation fields of shock wave therapy devicesJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:4f04159c-e0d0-4400-821c-899198421fafEnglishSymplectic Elements at Oxford2006Chitnis, PCleveland, RExtracorporeal shock wave therapy (ESWT) is considered a viable treatment modality for orthopedic ailments. Despite increasing clinical use, the mechanisms by which ESWT devices generate a therapeutic effect are not yet understood. The mechanistic differences in various devices and their efficacies might be dependent on their acoustic and cavitation outputs. We report acoustic and cavitation measurements of a number of different shock wave therapy devices. Two devices were electrohydraulic: one had a large reflector (HMT Ossatron) and the other was a hand-held source (HMT Evotron); the other device was a pneumatically driven device (EMS Swiss DolorClast Vet). Acoustic measurements were made using a fiber-optic probe hydrophone and a PVDF hydrophone. A dual passive cavitation detection system was used to monitor cavitation activity. Qualitative differences between these devices were also highlighted using a high-speed camera. We found that the Ossatron generated focused shock waves with a peak positive pressure around 40 MPa. The Evotron produced peak positive pressure around 20 MPa, however, its acoustic output appeared to be independent of the power setting of the device. The peak positive pressure from the DolorClast was about 5 MPa without a clear shock front. The DolorClast did not generate a focused acoustic field. Shadowgraph images show that the wave propagating from the DolorClast is planar and not focused in the vicinity of the hand-piece. All three devices produced measurable cavitation with a characteristic time (cavitation inception to bubble collapse) that varied between 95 and 209 μs for the Ossatron, between 59 and 283 μs for the Evotron, and between 195 and 431 μs for the DolorClast. The high-speed camera images show that the cavitation activity for the DolorClast is primarily restricted to the contact surface of the hand-piece. These data indicate that the devices studied here vary in acoustic and cavitation output, which may imply that the mechanisms by which they generate therapeutic effects are different. © 2006 American Institute of Physics. |
| spellingShingle | Chitnis, P Cleveland, R Acoustic and cavitation fields of shock wave therapy devices |
| title | Acoustic and cavitation fields of shock wave therapy devices |
| title_full | Acoustic and cavitation fields of shock wave therapy devices |
| title_fullStr | Acoustic and cavitation fields of shock wave therapy devices |
| title_full_unstemmed | Acoustic and cavitation fields of shock wave therapy devices |
| title_short | Acoustic and cavitation fields of shock wave therapy devices |
| title_sort | acoustic and cavitation fields of shock wave therapy devices |
| work_keys_str_mv | AT chitnisp acousticandcavitationfieldsofshockwavetherapydevices AT clevelandr acousticandcavitationfieldsofshockwavetherapydevices |