cardiovascular physiology jim pierce bi 145a lecture 14, 2009-10

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Cardiovascular Physiology Jim Pierce Jim Pierce Bi 145a Bi 145a Lecture 14, 2009-10 Lecture 14, 2009-10

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Page 1: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Cardiovascular Physiology

Jim PierceJim Pierce

Bi 145aBi 145a

Lecture 14, 2009-10Lecture 14, 2009-10

Page 2: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Arterial Blood Pressure:Escaped from the Heart

Page 3: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Blood Flow, Velocity, and Pressure

• We have talked about flow and velocity

• We know that flow and velocity are a function of the pressure gradient.

• Let’s consider Pressure.

Page 4: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Blood Pressure

• Pressure is force on an area

• If there is a fluid in a containerwe measure the pressure on the surface area of the container.

• That pressure is related to the number of particles that crash into that surface area per unit time

Page 5: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Blood Pressure

• Pressure in the reservoir is easy

– Since there is no net flow, the force on all sides of the reservoir is equal. Thus, measuring pressure anywhere measures pressure.

Page 6: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Blood Pressure

• Pressure in a pipe is hard

– Since there is net flow, there are fewer particles hitting the inflow area than the wall and more particles hitting the outflow area than the wall.

Page 7: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Blood Pressure

Page 8: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Blood Pressure

• There are two types of pressure:

• Static Pressure– Pressure from the blood distending the vessel

against the vascular smooth muscle– LaPlace: T=Pr (tension, pressure, radius)

Page 9: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Blood Pressure

• There are two types of pressure

• Dynamic Pressure– Pressure from the movement of particles along

the blood stream– Pitot: P=v2/2 (density, velocity)

Page 10: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Blood Pressure

Page 11: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Blood Pressure

• The Total Pressure is the sum of the static and dynamic pressures.

• This is much like Total Energy is the sum of the kinetic and potential energies.

Page 12: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Blood Pressure

• Where there is a high velocity (the aorta) there is a large component of “dynamic pressure” to the blood pressure.

• Where there is a low velocity (the peripheral arteries), the pressure is predominantly static.

Page 13: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Blood Pressure

• From a practical standpoint…

• THE blood pressure is what we measure if we stick a catheter into the lumen of a vessel and measure the outflow pressure.

Page 14: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Blood Pressure

Page 15: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Blood Pressure

• That is why we get away with our medical definition of “THE blood pressure”

• Regardless of the positioning of the catheter (intended to be along the middle of the blood vessel in line with outflow), we will see static pressure changes.

Page 16: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Blood Pressure Cuff

Page 17: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Afterload and Blood Pressure

• So when the heart produces aCardiac Output…

• It is putting FLOW into the Aorta

Page 18: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Afterload and Blood Pressure

• This FLOW has kinetic energy

• The energy of FLOW is converted into:– STATIC PRESSURE that stretches

the vessel walls– DYNAMIC PRESSURE of the blood moving

forward

Page 19: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Blood Velocity

This DECREASE in velocity reflects the ability of theAorta to ABSORB Static Pressure (i.e. store energy)

Page 20: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Afterload and Blood Pressure

• So AFTERLOAD = Vascular Resistance

• Blood Pressure reflects:– Cardiac Output (Flow = Total Energy)– Afterload (Vascular Resistance)

Page 21: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Afterload and Blood Pressure

• The take home point:

• Blood pressure is important becauseit gives information about:– The Heart Output– The Arterial Resistance

• But it is not Afterload

Page 22: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Blood Flow

• Preload is dominated by Cardiac Compliance

• Afterload is dominated byAortic Compliance

• Their relationship isCardiac Contractility

Page 23: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Blood Flow

• The heart takes Preload and converts it into flow against Afterload

• CO = HR * SV

• CO = BPsystemic / SVR

Page 24: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Womersley Number

• Dimensionless Number• Describes unsteady fluid flow resulting from an

unsteady pressure gradient.

• r=tube radius, f=frequency, n=order of harmonics, =fluid density, =viscosity index

fn

r

2

fn

r

2

fn

r

2

Page 25: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Womersley Number

• Dimensionless Number• Describes unsteady fluid flow resulting

from an unsteady pressure gradient.

• The Womersley Number is the “engineering” version of cardiac output

fn

r

2

fn

r

2

fn

r

2

Page 26: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

The Circuit

• Perfusate• Pump• Pipes

Page 27: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Systemic Blood Flow

• Everything before these organs is designed to maximize efficiency of cardiac output.– AORTA

• Everything leading to these organs is designed to regulate flow to the organs.– LARGE ARTERIES

• Everything leading to each vascular bed is designed to regulate flow inside the organs.– MEDIUM and SMALL ARTERIES

Page 28: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Microcirculation

AV Shunts andMetarteriolesdetermineCapillary flow.

Page 29: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Microcirculation

Page 30: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Microcirculation

Page 31: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

CapillaryNetworks

Page 32: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Capillary Endothelium

Page 33: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Microcirculation andFluid Movements

• There are two significant forces on the blood and fluid around the microcirculation

• There is a Hydrostatic Pressure

• There is an Oncotic Pressure

Page 34: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Microcirculation andFluid Movements

• The Hydrostatic Pressure– Is the pressure from fluid volume and flow

– Inside the blood vessel, it is ultimately derived from the work of the heart

– Outside the blood vessel, it is primarily derived from the presence of interstitial fluid trapped in the organ compartment.

Page 35: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Microcirculation andFluid Movements

• The Oncotic Pressure– Is the osmotic pressure of fluid and represents

the tendency to suck fluid in.

– Inside the blood vessel, it is derived from the plasma proteins (particularly albumin) and blood cells

– Outside the blood vessel, it is derived from the ground substance of the tissue

Page 36: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Microcirculation andFluid Movements

• Starling’s Law

• Qf = k [ (Pc+i) - (Pi + p) ]• Qf = net flow across membrane

• k = reflection coefficent (“fudge factor” like the rate constant or diffusion constant)

• Pc = Capillary Hydrostatic Pressure

• i = Interstital Fluid Oncotic Pressure

• Pi = Interstitial Fluid Hydrostatic Pressure

• p = Plasma Fluid Oncotic Pressure

Page 37: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Starling Forces in the Capillary Bed

Page 38: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Control of “Leakage”

• Different Endothelial phenotypes lead to different reflection coefficients (K)

Page 39: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Veins and Lymphatics

• Both are vascular systems for returning the perfusate to the heart.

• They are BOTH low pressure

• They are BOTH high compliance

Page 40: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Veins and Lymphatics

• The veins receive from the microcirculation

– Thus, the veins are part of a closed

cardiovascular system

– The veins receive blood

Page 41: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Veins and Lymphatics

• The lymphatics receive from the tissues

– Thus, the lymphatics are open

– The lymphatics receive interstitial fluid, or

ultrafiltrate, from the blood

Page 42: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Veins and Lymphatics

• Veins have a low venous resistance

• This determines flow rates across the hydrostatic pressure gradient between the microcirculation and the heart.

• Small change in resistance =Large change in compliance

Page 43: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Veins and Lymphatics

• Lymphatics have no actual resistance

• The mean tissue pressure is less than (or equal to) central venous pressure.

• Flow occurs by increases in tissue pressure above mean and valves to prevent backflow.

Page 44: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Veins and Lymphatics

• Veins drain into the large central veins, which act as the precardiac reservoir.

• Lymphatics drain to large lymphatic vessels which empty into the central venous system

– at the junction of internal jugular and subclavian veins.

Page 45: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Veins: From Small to Large

• Venules and Small Veins– Directly affect Starling Forces on Capillaries

• Medium Veins– Indirectly affect Tissue Bed Forces– Indirectly affect Cardiac Filling– Are the Largest Venous Reservoir of Blood

• Large Veins– Directly affect rate of Cardiac Filling

Page 46: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Special Circulations

• Cutaneous

• Splanchnic

• Portal Venous System

• Cerebral

• Coronary

• Fetal and Neonatal

Page 47: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Muscle Unit• Fascia wraps the “muscle meat”

• Tendon connects meat to bone

• Loose connective tissuesurrounds bunches of muscle

• Nerves and Vesselstravel between muscle

• Open ends of LymphaticVessels sit free inside the fascia compartment

Page 48: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Muscle Compartment

• Compartment Pressure– Generally 8-10 mmHg at rest– Can be affected by

• Inflow (Artery)

• Outflow (Vein and Lymphatic)

• Extravascular Volume– Extracellular Matrix

– Cell Volume

Page 49: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Connective Tissue

• Extracellular Matrix– Fibers

• Collagen• Elastin• Reticular Fibers

– Ground Substance• Blood Ultrafiltrate• Proteoglycans• Glycosaminoglycans

Page 50: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Body Fluids

• To understand ground substance,we must first talk about body waterand electrolytes

• Approximately 60% of the body is water.

Page 51: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Body Fluids

Page 52: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Body Fluids

• For a 70 kg man whose body read the book:

• Total Body Water = 42 Liters

• Intracellular Water = 28 Liters

• Extracellular Water = 14 Liters

Page 53: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Body Fluids

• Intracellular Fluid is easy:It’s all inside the cells

• Extracellular Fluid exists in two locations:– Intravascular (1/4 in blood vessels)– Interstitial (3/4 in tissues)

Page 54: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Body Fluids

Page 55: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Body Fluids

• What are the barriers between thesethree body spaces?– Intracellular– Interstitial– Intravascular

Page 56: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Body Fluids

• Between Intracellular and Interstitialis the CELL MEMBRANE

• Between Interstitial and Intravascularis the CAPILLARY MEMBRANE

Page 57: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Body Fluids

Page 58: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Body Fluids

• Why are these barriers important?Why are these barriers important?

• Only blood (intravascular) goesOnly blood (intravascular) goesto the kidney for processing.to the kidney for processing.

• The diffusion limitations of theseThe diffusion limitations of thesebarriers determine how accessiblebarriers determine how accessiblethings are to the kidneythings are to the kidney

Page 59: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Body Fluids

IntracellularInterstitialIntravascular

Page 60: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Body Fluids

• The body is not just “free water”

• There are many things that float around inside this water:

Page 61: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Body Fluids

• Proteins and their bound water• Small covalent compounds

– Some bound to protein (lipophilic)– Some with bound water

• Lipoproteins• Salts and their bound water

– Sodium, Chlorine– Bicarbonate

Page 62: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Interstitial Space

• The source of the Interstitial ECM is regional.The source of the Interstitial ECM is regional.

• Proteins (Fibers and Ground substance) often Proteins (Fibers and Ground substance) often come from the connective tissue cellscome from the connective tissue cells

• Salt, Water, and small molecules are Salt, Water, and small molecules are “Filtered” by the capillary membrane“Filtered” by the capillary membrane

• Waste Products are removed by theWaste Products are removed by theBlood and LymphaticsBlood and Lymphatics

• Hormones are produced and consumed Hormones are produced and consumed everywhere.everywhere.

Page 63: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Interstitial Space

• The source of the ICM is the Cell Itself.The source of the ICM is the Cell Itself.

• Proteins and Membranes are made.Proteins and Membranes are made.

• Salt, Water, and small molecules are Salt, Water, and small molecules are “Filtered” by the cell membrane. “Filtered” by the cell membrane.

Page 64: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Body Fluids

• Thus, the barriers determine the distribution Thus, the barriers determine the distribution of salts, small molecules, and waterof salts, small molecules, and water

• It is barrier function that maintainsIt is barrier function that maintainsthe differences between compartmentsthe differences between compartments

Page 65: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Body Fluids

Page 66: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Body Fluids

• Because the Capillary Membraneis rather “leaky”

• The Interstitialand Intravascularcompartments arequite similar

Page 67: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Body Fluids

• Because the Cell Membraneis not “leaky”

• The Interstitialand Intracellularcompartments are very different

Page 68: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Muscle Compartment

• Fluid Flux:– Blood comes in vi arteries– Both Osmosis and Diffusion occurs– Ultrafiltration produces Interstitial fluid

bathing Extracellular Matrix– Blood leaves via Veins– Interstitial fluid leaves via Lymphatics

Page 69: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Starling Forces in the Capillary Bed

Page 70: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Microcirculation andFluid Movements

• Starling’s Law

• Qf = k [ (Pc+i) - (Pi + p) ]• Qf = net flow across membrane

• k = reflection coefficent (“fudge factor” like the rate constant or diffusion constant)

• Pc = Capillary Hydrostatic Pressure

• i = Interstital Fluid Oncotic Pressure

• Pi = Interstitial Fluid Hydrostatic Pressure

• p = Plasma Fluid Oncotic Pressure

Page 71: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Muscle Compartment

• Mean arterial pressure – 32 mm Hg

• Mean venous pressure – 15 mm Hg

• Mean compartment pressure – 10 mm Hg

• Mean lymphatic pressure – 2 mm Hg

Page 72: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Starling Forces in the Capillary Bed

Page 73: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Glomerulus

• Fine Capillary Fine Capillary NetworkNetwork

Page 74: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Glomerular Filtration

Starling’s Forces are Starling’s Forces are alive and well in the capillary!alive and well in the capillary!

(They’re a little different, though)

Page 75: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

RBF and GFR

By controlling theBy controlling theafferent and efferentafferent and efferentarterioles, we controlarterioles, we control

Glomerular Filtration RateGlomerular Filtration Rate

Page 76: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

RBF and GFR

By controlling theBy controlling theafferent and efferentafferent and efferentarterioles, we also controlarterioles, we also control

Renal Blood FlowRenal Blood Flow

Page 77: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

RBF and GFR

Thus: the “arterial”Thus: the “arterial”nature of the glomerulusnature of the glomerulusallows us to apply steadyallows us to apply steadyhydrostatic pressurehydrostatic pressureacross the glomerulus,across the glomerulus,making a filtrate.making a filtrate.

Page 78: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Glomerular Membrane

• Made from:

– Endothelium– Basement

Membrane– Podocytes

The “Urine Filter”The “Urine Filter”

Page 79: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Glomerulus

• The endothelialmesh is coatedby cells called

Podocytes

Page 80: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Podocytes

Part of GlomerularMembrane

Page 81: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

TEM Podocytes

Page 82: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Glomerular Filter

• This filter has several effects because it is a gel:

– Its composition makes a “Pore Size”– Its composition makes a “Charge Barrier”

– (Just like gel electrophoresis)

Page 83: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Glomerular Filtration

Page 84: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Glomerular Filtration

Page 85: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Glomerular Filtration

Starling’s Forces are Starling’s Forces are alive and well in the capillary!alive and well in the capillary!

(They’re a little different, though)

Page 86: Cardiovascular Physiology Jim Pierce Bi 145a Lecture 14, 2009-10

Questions?