Proceedings of the International School of Physics "Enrico Fermi.", Volume 76N. Zanichelli, 1981 - Nuclear physics |
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Page 354
... stimulus intensity and the limit at which the CM is measured depends only on the experimental techniques used ... stimulus can elicit a d.c. potential change within the cochlea . This is the summating potential ( SP ) which to some ...
... stimulus intensity and the limit at which the CM is measured depends only on the experimental techniques used ... stimulus can elicit a d.c. potential change within the cochlea . This is the summating potential ( SP ) which to some ...
Page 356
... stimulus can be carried out by this place mechanism . How- ever , at low frequencies , below 100 Hz , the travelling wave extends over vir- tually the entire length of the basilar membrane and there is no clear max- imum in the wave ...
... stimulus can be carried out by this place mechanism . How- ever , at low frequencies , below 100 Hz , the travelling wave extends over vir- tually the entire length of the basilar membrane and there is no clear max- imum in the wave ...
Page 376
... stimulus generator provides the test signal , which is passed via attentuators to the output transducers such as loudspeakers , earphones or bone conductors . The stimulus generator should also provide masking noise and timing control ...
... stimulus generator provides the test signal , which is passed via attentuators to the output transducers such as loudspeakers , earphones or bone conductors . The stimulus generator should also provide masking noise and timing control ...
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