Proceedings of the International School of Physics "Enrico Fermi.", Volume 76N. Zanichelli, 1981 - Nuclear physics |
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Page 136
... zero everywhere and P , must at the same time be greater than P , due to the flow , and equal to P , and P , due to zero transmural pressure . This situation is unstable and a physically possible situation can only exist if we bring ...
... zero everywhere and P , must at the same time be greater than P , due to the flow , and equal to P , and P , due to zero transmural pressure . This situation is unstable and a physically possible situation can only exist if we bring ...
Page 154
... zero do we have the condition that P P. P. is meas- ured and follows P , with zero pressure difference . The all important question is thus how to reach a state of zero transmural pressure or , in other words , which is the « lock - on ...
... zero do we have the condition that P P. P. is meas- ured and follows P , with zero pressure difference . The all important question is thus how to reach a state of zero transmural pressure or , in other words , which is the « lock - on ...
Page 360
... zero dB level which has been evaluated by taking the statistical average of the hearing level of normal young persons . Hearing thresholds . within 20 dB of zero dB HL may be regarded as normal . When sounds are delivered , via an ...
... zero dB level which has been evaluated by taking the statistical average of the hearing level of normal young persons . Hearing thresholds . within 20 dB of zero dB HL may be regarded as normal . When sounds are delivered , via an ...
Contents
A R D THORNTON | 1 |
Physicists and clinicians | 5 |
The Fourier transform properties of an image | 12 |
Copyright | |
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alveolar amplitude analysis aorta aortic approximately arterial pressure arterial system attenuation value basilar membrane beam blood flow blood pressure C₁ capillary cardiac output circulation clinical cm³ CO₂ cochlea cochlear compartment compliance components computed tomography concentration constant counting rate cross-section cuff decrease detector diameter diastolic distribution effect elastin electrode energy equation filter fluid Fourier transform frame frequency function haemoglobin hair cells halothane heart rate impulse response increase left heart linear linear-attenuation coefficient lung manometer measured medical physics membrane method mmHg muscle normal obtained oxygen P₁ P₂ pacemaker patient peripheral resistance photons physicist physiological pulmonary pulsatile pulse ratio region Rendiconti S.I.F. sample scan scanner segment shown in fig shows signal stroke volume systolic techniques tissues transducer transmural pressure tube ultrasonic V₁ velocity venous system ventilation ventricle ventricular vessel viscoelastic volume wall wave form Windkessel X-ray zero