Peripheral circulation Flashcards
Capacitance and resistance:
Vascular capacitance is analogous to vascular resistance - but resistance refers to flow through a vessel, whereas capacitance relates to the volume that the vessel contains.
Changes in capacitance alter right ventricular filling and thus affect cardiac output.
The circulatory tree has multiple functions. It acts to:
Exchange O2 and CO2
Distribute nutrients to the cells of the body
Remove waste products of metabolism
Influence mean blood pressure and distribution of blood flow
Distribute endocrine secretions
Prevent bleeding or thrombosis
Combat infection
Regulate body temperature
What is the Windkessel effect
The arteries carry blood away from the heart and act as a hydraulic filter, ultimately converting the intermittent pulsatile ejection of blood from the heart into a steady flow with a constant pressure
Arterioles:
In arterioles, the small diameter provides a significant resistance to blood flow. This resistance ultimately determines the mean arterial blood pressure. Terminal arterioles provide the largest mean pressure drop (from 75 mmHg to 38 mmHg) of the normal circulation and provide about 70% of the vascular resistance.
Arterioles are normally in a state of partial vasoconstriction (tone) secondary to spontaneous contractile activity of the muscle wall and tonic sympathetic output. Systemic and local factors cause alterations in tone (degree of vasoconstriction), which in turn alters flow.
Venules:
Venules are post-capillary resistance vessels that regulate the capillary hydrostatic pressure.
Capillary hydrostatic pressure is one of the forces that determine the movement of water into and out of the intravascular and extracellular space. It is determined by the ratio of the resistances of the arterioles (pre-capillary resistance) and the venules (post-capillary resistance).
The smooth muscle tone of the post-capillary venules is controlled by the same systemic and local factors that control the tone of the arterioles. Though pre-capillary resistance influences the capillary hydrostatic pressure, the change in venous pressure has the greater effect.
Arteries and veins have the same three-layer structure:
Tunica intima (Fig 1a). This innermost layer is made up of a single layer of squamous endothelial cells surrounded by a thin layer of subendothelial connective tissue
Tunica media (Fig 1b). This layer contains circularly arranged elastic fibres and connective tissue and the vascular smooth muscle which controls the diameter of the vessel
Tunica adventitia (Fig 1c). This outermost layer is made up entirely of connective tissue and contains the nerves that supply the vessel and, in larger vessels, the vasa vasorum
What do you think is the velocity of pulsatile flow at the level of the ascending aorta?
At the level of the ascending aorta the velocity of pulsatile flow is about 1 m/s.
As the stroke volume enters the aorta, the aorta expands. Elastic recoil during diastole acts to smooth out the pulsatile nature of the heart’s pumping action (Windkessel effect).
As arteries divide and divide again, the total cross-sectional area increases, so the mean blood pressure and velocity fall. When the blood arrives at the capillary exchange beds, flow is smooth and slow, and pressure is low. Thus the role of the arterial system is to convert the high-velocity pulsatile flow, at the level of the ascending aorta, to the optimal low-velocity steady flow in the capillary bed (around 0.01 cm/s) that is necessary for cellular exchanges
Throughout the vascular tree, the endothelium has a number of functions including:
Regulating basal vasomotor tone (and hence, blood pressure) by the controlled release of:
-vasodilators, i.e. nitric oxide (NO) and prostaglandin I2 (PGI2, prostacyclin)
-vasoconstrictors, i.e. endothelins and platelet activating factor (PAF)
Acting as a non-thrombogenic surface, secondary to expressing heparan sulphate, protein C and protein S.
Presenting a smooth surface to encourage laminar flow
Regulating the growth of surrounding connective tissue
The capillary endothelium:
Unlike arteries and veins, capillaries (5-10 μm diameter) consist of just a single layer of endothelium and some connective tissue. These cells form a semipermeable or selectively permeable membrane which allows the diffusion of fluids, nutrients and waste products between the lumen of the capillary and the surrounding tissue. To increase permeability, the cells of the capillary endothelium are thinner than those of the arteries and veins.
There are three types of capillary depending on the arrangement of their endothelial cells:
1) Continuous - where endothelial cells form an uninterrupted (continuous) lining, e.g. in the brain, so that only water, gases and ions diffuse through the intercellular clefts or tight junctions
2) Fenestrated - where pores allow small molecules to diffuse
3) Sinusoidal - in the bone marrow and liver, where larger proteins and even white and red cells pass through
What is third spacing?
In disease states, e.g. sepsis, vascular permeability increases. This increased ‘leakiness’ is sometimes referred to as ‘third spacing’ or ‘third space losses’. It is mediated by histamine, prostaglandins and interleukins. Oedema results when this increased fluid and protein loss overwhelms the absorptive capacity of the lymphatic system.
Where is the permeability of a capillary greatest?
Along the length of an individual capillary, permeability is greatest at the venous end of the capillary
Poiseuille’s Equation
Flow (Q) = pi(P2-P1)r^4/ 8nl
P2-P1 = pressure difference
r= radius
n= viscosity
l= length
Flow of any liquid proceeds from a point of higher pressure to one of lower pressure.
The total flow is determined by:
The pressure gradient
The length of the vessel
The radius of the vessel
The viscosity of the fluid
Poiseuille described this relationship mathematically by studying the flow of a homogenous (Newtonian) fluid through rigid, uniform, non-branching glass tubes.
What is resistance characterised by?
The diameter and, to a lesser extent, the length of an individual vessel
The organization of the vascular network (in series or in parallel)
The physical characteristics of the blood itself (viscosity)
The type of flow (turbulent or laminar)
Within a single vessel, hydraulic resistance to flow is determined by vessel diameter or radius, vessel length and the viscosity of the blood.
Resistance equation:
R= 8nl/ pi x r^4
Mathematically then R varies directly with viscosity (η) and length (l) and inversely with the fourth power of the radius (r).
Vessel diameter - specifically of the arterioles, the ‘resistance’ vessels - is the single most important factor in controlling distribution of flow and determining mean blood pressure. Because flow directly affects oxygen delivery, any change in arteriolar diameter enables flow to tissues to be adjusted to match metabolic requirements.
What would be the difference in resistance in two tubes of the same radius, if one is twice the length of the other?
you can deduce that a vessel that has twice the length of another vessel (that has the same radius) has twice the resistance to flow (Fig 2).
However, under physiological conditions, vessel length does not change significantly and blood viscosity usually stays within a small range (except when haematocrit changes). Therefore, although resistance varies directly with η and l, both are relatively fixed values in the circulation, and have little effect on resistance.
How would a 2-fold increase in radius (r) affect resistance?
Resistance varies inversely with r4, so a 2-fold increase in r would decrease resistance 16-fold (Fig 3). A 4-fold in r would decrease resistance (R) 256-fold. By extension, flow would increase 16 and 256 times respectively.
In contrast to η and l, resistance is extremely sensitive to changes in r. Changing the radius of a vessel by contraction or relaxation of its smooth muscle profoundly alters the resistance to flow, and therefore, drugs or other modulating factors which dilate or constrict the vessels have a powerful effect on blood flow.
Resistance in series
If across each serial resistance (Fig 1a):
The driving pressure (ΔP) is 3 mmHg and
The flow (Q) is 1 ml/min
then:
For each resistance R = ΔP/Q or 3 mmHg/ml/min, and
The total resistance of the series is Rs = 9 mmHg/ml/min
Parallel resistance
In parallel resistances (Fig 1b), if the values are the same across each resistance,
ΔP is 3 mmHg and Q is 1 ml/min, then the total resistance is
1/Rp = 1/R1 + 1/R2 + 1/R3 or 1 mmHg/ml/min
In this example, Rp is only 1/9 of that of the same three resistances in series (i.e. the ratio of Rp/Rs = 1/9).
From this it can be deduced that for parallel resistances, it takes a ΔP of only 1 mmHg (instead of 9 mmHg for series resistances) to produce a flow of 1 ml/min.
Differentiate between the terms ‘velocity’ and ‘flow’:
Velocity (v) is the distance the blood moves with respect to time, usually expressed in cm/s
Flow is the volume of blood moving per unit of time, expressed as ml/min or cm3/min
How is the flow of blood in a vessel related to velocity?
Q = vA, where A is the cross-sectional area of the vessel.
Thus velocity is low where the area is large and high where the area is small (Fig 1).
To illustrate, the smallest cross-sectional area to receive the entire stroke volume is the aorta (~2.5 cm2) where velocity of flow is highest at 0.93 m/s. As arteries divide into smaller and smaller vessels, the total cross-sectional area increases and blood velocity falls. In the capillaries, where the total cross-sectional area is 1000 times that of the aorta, flow is 0.05 cm/s. This slowing of blood velocity enables efficient exchange of gases and metabolites across the short length of capillaries.
The relationship between flow in a tube (rather than velocity) and area is more complex and is described by Poiseuille’s Law.
What is laminar flow?
Laminar flow describes fluid where all the elements of the fluid move in streamlined layers parallel to the vessel wall. The central core of fluid has the highest velocity and each cylinder of fluid around this central column is progressively slower until the outermost layer, in contact with the vessel wall is stationary. The profile of flow velocity across the tube forms a parabola (Fig 2).
The ease with which each ‘layer’ of fluid slides over its neighbour is determined by the fluid viscosity. The higher the fluid viscosity, the less slippery the fluid is and flow is reduced for any given pressure.
What is turbulent flow?
Where the blood velocity is high, a point is reached at which flow is no longer directly proportional to pressure. This happens because flow is no longer laminar, but turbulent (Fig 3). In turbulent flow, fluid moves in discordant eddies and the frictional resistance to flow increases. In the ascending aorta (velocity 0.93 cm/s), flow is turbulent, and will only increase in proportion to the square root of pressure.
Describe Reynold’s number and its importance in the pressure-flow relationship:
Reynolds number is used to determine whether flow is likely to be laminar or turbulent by identifying the point when flow is no longer proportional to the driving pressure (Fig 1):
Laminar flow, which is characterized by smooth fluid motion, occurs at low Reynolds numbers, where viscous forces predominate
Turbulent flow occurs at high Reynolds numbers and is dominated by inertial forces, which tend to produce chaotic eddies, vortices and other flow instabilities
What is the equation for turbulent flow?
Poiseuille’s law on pressure-flow relationships in the circulation depends on conditions of laminar flow for accuracy. When flow becomes turbulent, Poiseuille’s law no longer holds, and the flow rate becomes proportional to the square root of the pressure gradient, rather than being directly proportional to pressure gradient. In turbulent flow:
Q ∝ √ΔP
Turbulence increases the energy required to drive blood flow because turbulence increases friction.
Additionally, the pressure drops seen through tubes can be predicted by plotting the wall friction factor f against Reynolds number Re. The relative roughness of the vessel thus plays a part in pressure-flow predictions.
Blood viscosity is affected by:
Haematocrit
Temperature
Vessel diameter
Flow rate