1955
DOI: 10.1113/jphysiol.1955.sp005330
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Velocity profiles of oscillating arterial flow, with some calculations of viscous drag and the Reynolds number

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Cited by 133 publications
(61 citation statements)
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“…The red blood cell velocity distribution in a conduit artery at rest varies between the cardiosystolic and the cardiodiastolic phase [1][2][3][4]. In the carotid and femoral arteries at rest, it has previously been demonstrated that the blood velocity profile during the cardiosystolic phase is less "steep" and somewhat more "flat" compared to the "steeper" parabolic velocity profile during the cardiodiastolic phase [4][5][6].…”
mentioning
confidence: 99%
“…The red blood cell velocity distribution in a conduit artery at rest varies between the cardiosystolic and the cardiodiastolic phase [1][2][3][4]. In the carotid and femoral arteries at rest, it has previously been demonstrated that the blood velocity profile during the cardiosystolic phase is less "steep" and somewhat more "flat" compared to the "steeper" parabolic velocity profile during the cardiodiastolic phase [4][5][6].…”
mentioning
confidence: 99%
“…For the capillary tube model, pulsatile flow has been characterized using the Womersley model to calculate shear stress [20,68]. However, some have reported values for FSS in unsteady flow regimes without including their methods of calculation [18].…”
Section: Huvec Protein Expression (Properdin)mentioning
confidence: 99%
“…When unsteady flows are outside this regime, they showed that FSS can be calculated using a similar derivation to Womersley's solution for unsteady flow in a rigid tube [10,20]. Hsiai et al demonstrated another approach: measuring heat transfer at the wall directly by using MEMS sensors, then calculating the FSS based on heat transfer principles [21].…”
Section: Introductionmentioning
confidence: 99%
“…It is concluded that the Womersley number, a, a dimensionless expression of the pulsatile flow frequency in relation to viscous effects, is the only parameter that governs the behaviour of oscillatory flow and that the wave speed increases with the Womersley number tending to an asymptotic value obtained by Lamb (1898). The model predicts the phase lag between the pressure gradient and the flow as well as flow reversal initiating at the walls (Hale et al, 1955). A second two-dimensional algorithm was proposed by Branson (1945).…”
Section: Introductionmentioning
confidence: 99%