FUNCTION
OF THE VASCULAR SYSTEM
The
amount of blood flow needed by body tissues constantly changes. The percentage
of blood flow received by individual or-gans or tissues is determined by the
rate of tissue metabolism, the availability of oxygen, and the function of the
tissues (Table 31-1). When metabolic requirements increase, blood vessels
dilate to in-crease the flow of oxygen and nutrients to the tissues. When
metabolic needs decrease, vessels constrict, and blood flow to the tissues
decreases. Metabolic demands of tissues increase with physical activity or
exercise, local heat application, fever, and in-fection. Reduced metabolic
requirements of tissues accompany rest or decreased physical activity, local
cold application, and cooling of the body. If the blood vessels fail to dilate
in response to the need for increased blood flow, tissue ischemia (ie, deficient blood supply to a body part) results. The
mechanism by which blood vessels dilate and constrict to adjust for metabolic
changes ensures that normal arterial pressure is maintained.
As
blood passes through tissue capillaries, oxygen is removed, and carbon dioxide
is added. The amount of oxygen extracted by each tissue differs. For example,
the myocardium tends to extract about 50% of the oxygen from arterial blood in
one pass through its capillary bed, whereas the kidneys extract only about 7%
of the oxygen from the blood that passes through them. The aver-age amount of
oxygen removed collectively by all of the body tis-sues is about 25%. This
means that the blood in the vena cavae contains about 25% less oxygen than
aortic blood. This is known as the systemic
arteriovenous oxygen difference. The value increases when the amount of
oxygen delivered to the tissues is decreased relative to their metabolic needs
(see Table 31-1).
Blood
flow through the cardiovascular system always proceeds in the same direction:
left side of the heart to the aorta, arteries, ar-terioles, capillaries,
venules, veins, vena cavae, and right side of the heart. This unidirectional
flow is caused by a pressure differ-ence that exists between the arterial and
venous systems. Because arterial pressure (approximately 100 mm Hg) is greater
than ve-nous pressure (approximately 4 mm Hg) and fluid always flows from an
area of high pressure to an area of lower pressure, blood flows from the
arterial to the venous system.
The
pressure difference (∆P) between the two ends
of the ves-sel provides the impetus for the forward propulsion of blood.
Im-pediments to blood flow offer the opposing force, which is known as
resistance (R). The rate of blood flow is determined by dividing the pressure
difference by the resistance:
Flow
rate =∆P/R
This
equation clearly shows that, when resistance increases, a greater driving
pressure is required to maintain the same degree of flow. In the body, an
increase in driving pressure is accom-plished by an increase in the force of
contraction of the heart. If arterial resistance is chronically elevated, the
myocardium hyper-trophies (enlarges) to sustain the greater contractile force.
In
most long smooth blood vessels, flow is laminar or stream-lined, with blood in
the center of the vessel moving slightly faster than the blood near the vessel
walls. Laminar flow becomes tur-bulent when the blood flow rate increases, when
blood viscosity increases, when the diameter of the vessel becomes greater than
normal, or when segments of the vessel are narrowed or con-stricted. Turbulent
blood flow creates a sound, called a bruit,
that can be auscultated with a stethoscope.
Fluid
exchange across the capillary wall is continuous. This fluid, which has the
same composition as plasma without the proteins, forms the interstitial fluid.
The equilibrium between hydrostatic and osmotic forces of the blood and
interstitium, as well as cap-illary permeability, governs the amount and
direction of fluid movement across the capillary. Hydrostatic force is a
driving pres-sure that is generated by the blood pressure. Osmotic pressure is
the pulling force created by plasma proteins. Normally, the hy-drostatic
pressure at the arterial end of the capillary is relatively high compared with
that at the venous end. This high pressure at the arterial end of the
capillaries tends to drive fluid out of the capillary and into the tissue
space. Osmotic pressure tends to pull fluid back into the capillary from the
tissue space, but this os-motic force cannot overcome the high hydrostatic
pressure at the arterial end of the capillary. At the venous end of the
capillary, however, the osmotic force predominates over the low hydro-static
pressure, and there is a net reabsorption of fluid from the tissue space back
into the capillary.
Except
for a very small amount, fluid that is filtered out at the arterial end of the
capillary bed is reabsorbed at the venous end. The excess filtered fluid enters
the lymphatic circulation. These processes of filtration, reabsorption, and
lymph formation aid in maintaining tissue fluid volume and removing tissue
waste and debris. Under normal conditions, capillary permeability remains
constant.
Under
certain abnormal conditions, the fluid filtered out of the capillaries may
greatly exceed the amounts reabsorbed and car ried away by the lymphatic
vessels. This imbalance can result from damage to capillary walls and
subsequent increased permeability, obstruction of lymphatic drainage, elevation
of venous pressure, or decrease in plasma protein osmotic force. The
accumulation of fluid that results from these processes is known as edema.
The
most important factor that determines resistance in the vas-cular system is the
vessel radius. Small changes in vessel radius lead to large changes in
resistance. The predominant sites of change in the caliber or width of blood
vessels, and therefore in resistance, are the arterioles and the precapillary
sphincter. Pe-ripheral vascular resistance is the opposition to blood flow
pro-vided by the blood vessels. Poiseuille’s law provides the method by which
resistance can be calculated:
R = 8θL/πr4
where
R = resistance, r = radius of the vessel, L
= length of the vessel, θ
=
viscosity of the blood, and 8/Ï€ = a constant. This
equa-tion shows that the resistance is proportional to the viscosity or
thickness of the blood and the length of the vessel but is inversely
proportional to the fourth power of the vessel radius.
Under
normal conditions, blood viscosity and vessel length do not change
significantly, and these factors do not usually play an important role in blood
flow. A large increase in hematocrit, how-ever, may increase blood viscosity
and reduce capillary blood flow.
Because
the metabolic needs of body tissues, even at rest, are con-tinuously changing,
an integrated and coordinated regulatory sys-tem is necessary so that blood
flow to individual areas is maintained in proportion to the needs of that area.
As might be expected, this regulatory mechanism is complex and consists of
central nervous system influences, circulating hormones and chemicals, and
inde-pendent activity of the arterial wall itself.
Sympathetic
(adrenergic) nervous system activity, mediated by the hypothalamus, is the most
important factor in regulating the caliber and therefore the blood flow of
peripheral blood vessels. All vessels are innervated by the sympathetic nervous
system except the capillary and precapillary sphincters. Stimulation of the
sympa-thetic nervous system causes vasoconstriction. The neurotransmit-ter
responsible for sympathetic vasoconstriction is norepinephrine. Sympathetic
activation occurs in response to physiologic and psy-chological stressors.
Diminution of sympathetic activity by med-ications or sympathectomy results in
vasodilation.
Other
hormonal substances affect peripheral vascular resis-tance. Epinephrine,
released from the adrenal medulla, acts like norepinephrine in constricting
peripheral blood vessels in most tissue beds. In low concentrations, however,
epinephrine causes vasodilation in skeletal muscles, the heart, and the brain.
Angio-tensin, a potent substance formed from the interaction of renin
(synthesized by the kidney) and a circulating serum protein, stim-ulates
arterial constriction. Although the amount of angiotensin concentrated in the
blood is usually small, its profound vasocon-strictor effects are important in
certain abnormal states, such as heart failure and hypovolemia.
Alterations
in local blood flow are influenced by various circu-lating substances that have
vasoactive properties. Potent vaso-dilators include histamine, bradykinin,
prostaglandin, and certain muscle metabolites. A reduction in available oxygen
and nutrients and changes in local pH also affect local blood flow. Serotonin,
a substance liberated from platelets that aggregate at the site of ves-sel wall
damage, constricts arterioles. The application of heat to parts of the body
surface causes local vasodilation, whereas the application of cold causes
vasoconstriction.
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