Презентация на тему: Haemodynamics Haemorheology

Haemodynamics Haemorheology Branches of physics Branches of physics Laminar and turbulent flow V iscosity V iscosity Newton's Law of Viscosity Haemodynamics Haemorheology Reynolds number Reynolds number Reynolds number Pascal's law Bernoulli's principle Hagen–Poiseuille law Hagen–Poiseuille law Cardiac output Major factors influencing cardiac output Frank–Starling law Myocardial contractility Preload Afterload Vascular resistance Rouleaux Rouleaux Rouleaux Rouleaux Hagen–Poiseuille law Now summarize three major concepts presented in this lecture
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Первый слайд презентации: Haemodynamics Haemorheology

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Слайд 2: Branches of physics

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Слайд 3: Branches of physics

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Слайд 4: Laminar and turbulent flow

(a) occurs when a fluid flows in parallel layers, with no disruption between the layers (b) is a flow regime that demonstrates chaotic changes in pressure and flow velocity

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Слайд 5: V iscosity

The viscosity of a fluid is a measure of its resistance to gradual deformation by shear stress or tensile stress

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Слайд 6: V iscosity

Viscosity is a property of the fluid which opposes the relative motion between the two surfaces of the fluid that are moving at different velocities. When the fluid is forced through a tube, the particles which compose the fluid generally move more quickly near the tube's axis and more slowly near its walls; therefore some stress is needed to overcome the friction between particle layers to keep the fluid moving.

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Слайд 7: Newton's Law of Viscosity

F is the shear stress in the fluid η is a scalar constant of proportionality, the shear viscosity of the fluid dV/dZ is the derivative of the velocity component that is parallel to the direction of shear, relative to displacement in the perpendicular direction. S is the surface (area) between fluid and the tube.

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Слайд 8

Newtonian fluid fluid in which the viscous stresses arising from its flow, at every point, are linearly proportional to the local strain rate ( the rate of change of its deformation over time ). Non- Newtonian fluid viscosity is dependent on shear rate or shear rate history. Shear thickening (dilatant) - a pparent viscosity increases with increased stress. Shear thinning (pseudoplastic) - a pparent viscosity decreases with increased stress

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Слайд 9: Reynolds number

Is the important dimensionless quantity refers to ratio of inertial forces to viscous forces within a fluid which is subjected to relative internal movement due to different fluid velocities, in which is known as a boundary layer in the case of a bounding surface such as the interior of a pipe.

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Слайд 10: Reynolds number

U sed to help predict flow patterns in different fluid flow situations. At low Reynolds numbers viscous forces are dominant, and is characterized by smooth, constant fluid motion ( laminar flow ). A t high Reynolds numbers flow is dominated by inertial forces, which tend to produce chaotic eddies, vortices and other flow instabilities ( turbulen t flow).

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Слайд 11: Reynolds number

where in : v s - mean fluid velocity, [m / s] L - characteristic length, [m] μ - (absolute) dynamic fluid viscosity, [Pa * s] ν - kinematic fluid viscosity: ν = μ / ρ, [m² / s] ρ - fluid density, [kg * m -3 ]

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Слайд 12: Pascal's law

Pascal's law is a principle in fluid mechanics that states that a pressure change occurring anywhere in a confined incompressible fluid is transmitted throughout the fluid such that the same change occurs everywhere

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Слайд 13: Bernoulli's principle

ρv 2 /2 + ρgh + p = const ρv 2 /2 is dynamic pressure, ρgh is hydraulic head p = static pressure

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Слайд 14: Hagen–Poiseuille law

flow of liquid depends on following factors: like the pressure gradient (∆P), the length of the narrow tube (L) of radius (r) and the viscosity of the fluid ( η ) along with relationship among them. Q = Δ P π r 4 /8 η L Assumptions: The tube is stiff, straight, and uniform Liquid is Newtonian, i.e., viscosity is constant The flow is laminar and steady, not pulsatile, and the velocity at the wall is zero (no slip at the wall)

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Слайд 15: Hagen–Poiseuille law

The Pressure Gradient (∆P) : Shows the difference in the pressure between the two ends of the tube, determined by the fact that any fluid will always flow from high pressure to low pressure region and the flow rate is determined by the pressure gradient ( ΔP = P 1 – P 2 ) Radius of tube : The liquid flow varies directly with the radius to the power 4. Viscosity ( η ) : The flow of the fluid varies inversely with the viscosity of the fluid and as the viscosity of the fluid increases, the flow decreases vice versa. Length of the Tube (L): The liquid flow is inversely proportional to the length of the tube, therefore longer the tube, greater is the resistance to the flow. Resistance(R): The resistance is described by 8 η L/ π r4 and therefore the Poiseuille’s law becomes Q = Δ P π r 4 / 8 η L Q= (ΔP) / R

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Слайд 16: Cardiac output

Is the volume of blood being pumped by the heart, in particular by the left or right ventricle, per unit time. CO = HR × SV

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Слайд 17: Major factors influencing cardiac output

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Слайд 18: Frank–Starling law

The Frank–Starling law of the heart represents the relationship between stroke volume and end diastolic volume. The law states that the stroke volume of the heart increases in response to an increase in the volume of blood in the ventricles, before contraction (the end diastolic volume), when all other factors remain constant. As a larger volume of blood flows into the ventricle, the blood stretches the cardiac muscle fibers, leading to an increase in the force of contraction.

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Слайд 19: Myocardial contractility

This results in better ejection of the blood in the ventricles. Controlled by extrinsic factors sympathetic stimulation of the heart hormones K+ and Ca++ channel blockers Myocardial contractility (c ardiac i notropy ) represents the innate ability of the heart muscle to contract. Changes in the ability to produce force during contraction result from incremental degrees of binding between thick and thin filaments.

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Слайд 20: Preload

P reload is the end diastolic volume that stretches the right or left ventricle of the heart to its greatest dimensions under variable physiologic demand. I t is the initial stretching of the cardiomyocytes prior to contraction; therefore, it is related to the sarcomere length at the end of diastole.

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Слайд 21: Afterload

Afterload is the stress in the wall of the left ventricle during ejection. I t is the end load against which the heart contracts to eject blood. Afterload is readily broken into components: one factor is the aortic pressure / pulmonary pressure the left /right ventricular muscle must overcome to eject blood.

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Слайд 22: Vascular resistance

Vascular resistance is the resistance that must be overcome to push blood through the circulatory system and create flow. Resistance is a factor of: Blood v iscosity Total b lood v essel l ength Vessel d iameter

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Слайд 23: Rouleaux

Rouleaux are stacks or aggregations of red blood cells which form because of the unique discoid shape of the cells in vertebrates. The flat surface of the discoid RBCs gives them a large surface area to make contact with and stick to each other; thus forming a rouleau.

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Слайд 24: Rouleaux

Diameter of blood vessel is more than diameter of rouleaux

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Слайд 25: Rouleaux

Diameter of blood vessel is nearly equal to diameter of rouleaux

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Слайд 26: Rouleaux

Diameter of blood vessel is less than diameter of RBC

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Слайд 27: Hagen–Poiseuille law

Pressure gradient: created by the heart. Resistance Radius of tube: diameter of blood vessels. Viscosity : property of blood. Length of the tube Q = Δ P π r 4 / 8 η L Q= (ΔP) / R

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