Please use this identifier to cite or link to this item: https://hdl.handle.net/20.500.14279/1135
DC FieldValueLanguage
dc.contributor.authorBlowes, R. W.-
dc.contributor.authorMilner, Anthony David-
dc.contributor.authorYiallouros, Panayiotis K.-
dc.contributor.otherΓιάλλουρος, Παναγιώτης-
dc.date.accessioned2015-04-20T08:38:43Z-
dc.date.accessioned2015-12-02T08:50:49Z-
dc.date.available2015-04-20T08:38:43Z-
dc.date.available2015-12-02T08:50:49Z-
dc.date.issued1995-06-
dc.identifier.citationPediatric Pulmonology, 1995, vol. 19, no. 6, pp. 348-354en_US
dc.identifier.issn10990496-
dc.identifier.urihttps://hdl.handle.net/20.500.14279/1135-
dc.description.abstractPrevious studies have reported great difficulty in recording lung sounds from neonates and have found conflicting results. We studied lung sounds in neonates during the inspiratory phase of the respiratory cycle as monitored by inductive plethysmography (A) and by pneumotachograph and face mask (8) which added dead space of 12 mL. Sixteen term babies were tested 12 hr to 6 days (median 45 hours) after birth. Lung sounds were recorded and then analysed using overlapping and nonoverlapping fast Fourier transforms. The two methods of analysis showed difference in intensity but not in frequency. Fourteen babies provided enough breaths for comparison; total of 596 inspirations were analysed. The intensity of lung sounds on occasion B was higher in all but two babies with mean B/A ratio of 2.4. The mean (SD) power on occasions A and B was 13.9(8.5) mW and 26.9 (21.0) mW, P = 0.02, respectively. In all but 4 babies the B/A ratios of the median (f50) and 90th centile (f90) frequencies were scattered randomly within 20% of unity. The mean (SD) f50 on occasions A and B was 205.5 (51.1) Hz and 225.8 (32.3) Hz, P = 0.10, respectively; the mean f50 was 370.3 (91.0) Hz and 396.1 (67.8) Hz, P = 0.25, respectively. Linear regression showed that there is third-order polynomial relationship between sound intensity and air flow at the mouth. A weaker positive association exists between frequency and air flow, showing that the median and 90th centile frequencies approach an asymptote as flow increases. We conclude that adding dead space increases the intensity of lung sounds in neonates due to increased flow, but has no consistent effect on frequency content.en_US
dc.formatpdfen_US
dc.language.isoenen_US
dc.relation.ispartofPediatric Pulmonologyen_US
dc.rights© Wileyen_US
dc.subjectLung soundsen_US
dc.subjectNeonatesen_US
dc.subjectAuscultationen_US
dc.titleLung sounds in neonates with and without an added dead spaceen_US
dc.typeArticleen_US
dc.collaborationSt. Thomas' Hospitalen_US
dc.subject.categoryClinical Medicineen_US
dc.journalsSubscriptionen_US
dc.reviewPeer Revieweden
dc.countryUnited Kingdomen_US
dc.subject.fieldMedical and Health Sciencesen_US
dc.publicationPeer Revieweden_US
dc.identifier.doi10.1002/ppul.1950190607en_US
dc.dept.handle123456789/54en
dc.relation.issue6en_US
dc.relation.volume19en_US
cut.common.academicyear2020-2021en_US
dc.identifier.spage348en_US
dc.identifier.epage354en_US
item.fulltextNo Fulltext-
item.cerifentitytypePublications-
item.grantfulltextnone-
item.openairecristypehttp://purl.org/coar/resource_type/c_6501-
item.openairetypearticle-
item.languageiso639-1en-
crisitem.journal.journalissn1099-0496-
crisitem.journal.publisherWiley-
crisitem.author.deptCyprus International Institute for Environmental and Public Health-
crisitem.author.facultyFaculty of Health Sciences-
crisitem.author.orcid0000-0002-8339-9285-
crisitem.author.parentorgFaculty of Health Sciences-
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