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Dr .Lakshmi Gopalakrishnan Southern Railway Hospital
Cathlab hemodynamics – 1 pressures, waveforms ,cardiac output and resistance Dr .Lakshmi Gopalakrishnan Southern Railway Hospital
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HEMODYNAMICS IN CARDIAC CATHETERIZATION
PRESSURE MEASUREMENTS MEASUREMENT OF FLOW VASCULAR RESISTANCE Principle of Ohm’s Law : Q = ∆ P / R
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Pressure recording system
Consists of catheter , transducer, amplifier and recorder Must meet : amplitude linearity adequate frequency response phase linearity calibration of transducer over range of amplitudes,and a plot gives linear relationship optimal damping
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Frequency response and optimal damping
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Pressure Measurement systems
Fluid filled catheters Micromanometer catheters
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Transducers – to be calibrated against a known pressure, “ zeroed” placing at mid chest level and balanced ( zero all the transducers being used simultaneously) immediately prior to obtaining simultaneous recordings
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Fluid filled system - contd
Sources of error Distortion of the output signal due to frequency response and damping charecteristics optimal damping achieved by short, wide-bore , non compliant catheter directly connected to transducer with no air bubbles in the liquid .This achieves frequency response close to output –to-input ratio of 1. catheter whip artifact, end-pressure artifact, catheter impact artifact, catheter tip obstruction
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Pressure measurement – micromanometer system
Advantages include higher natural frequencies, optimal damping characteristics, no whip artifacts Less distorsion of waveforms, lack the msec delay Commercially available ones have both end hole and side holes for over the wire use and angiography and ones with two tip transducers for pressure gradients Disadvantages - expense, fragility, added procedure time Used for research work only.
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Fluid filled catheter vs micromanometer catheter
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Normal pressure waveforms
Atrial waveforms Right atrium a wave highest Pre – a wave pressure a wave x descent x’ descent v wave y descent Left atrium v wave highest , pressure higher Pulmonary capillary wedge, similar to LA waveform, damped, delayed
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Respiratory variation
During spontaneous respiration intrathoracic pressure falls in end expiration by 3-4 mmhg and end-inspiration by 7-8 mmhg This reduces the RA, LA, Aortic pressures and hence underestimates All recordings in end expiration since it closely resembles the atmospheric pressure
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Atrial waveforms- important points
Shows two positive waves ‘a’ atrial and ‘v’ ventricular and negative waves x’ and y descents ‘a’ wave is prominent with abnormalities of reduced RV,LV compliance ‘v’ wave is prominent in AV valve regurgitation X’ and y descents are diminished in pericardial tamponade X’ and y descents are accentuated in constriction and restrictive diseases
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Ventricular pressure waveform
Consists of Small rapid-filling wave slow filling wave ‘a’ wave co-incident with atrial systole Ventricular systolic pressure wave Pressures reported are early diastolic pressure End- diastolic pressure peak systolic pressure
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Ventricular pressure waveform -- diastole
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Ventricular pressure waveform - systole
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Arterial pressure waveforms
Rapidly rising systolic pulse wave ‘ incisura’ End diastolic pressure Measured central aortic pressure wave is a conjugate of both forward and reflected waves factors that augment pressure wave reflections vasoconstriction heart failure hypertension ilio femoral obstruction valsalva – after release
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Aortic pressure waveform
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Central aortic pressure waveform a conjugate of forward & reflected waves
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Aortic pressure waveforms as a function of distance from the Aortic valve
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from augmentation of reflected waves
Aortic pressure waveform before & after occlusion of femoral –major increase from augmentation of reflected waves
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Pulmonary artery pressure waveform
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Cardiac output Quantity of blood supplied to systemic circulation per unit time in L / min Determined by preload, heart rate and myocardial contractility Cardiac index = CO in L / min / m2 BSA Other variables like age, posture, temperature considered while interpreting CO
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Determination of CO - Technique
Fick’s oxygen method Thermodilution method Fick’s principle- states that the total uptake or release of any substance by an organ is the product of blood flow to the organ and the art- venous concentration difference of the substance CO = O2 consumption / AV Oxygen difference CO = x BSA (Sa O2 – Sv O2) x Hb x 1.36 x 10 Error in this method -10% Most accurate in low output states and conditions with irregular HR like AF and V bigeminy
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Thermodilution method
Injection of 10ml of cold saline in the Right atrium Measure the temp change in the PA and a transient drop in temp occurs Curve plotted of the temp of PA vs time Has a smooth up slope and a more gentle decline Area under the curve is inversely proportional to the CO CO = CC x (Tb – Ti). Where cc is the computation constant, Tb the blood temperature and Ti the injectate temperature Severe TR is a contraindication to use of the method Error with this method 5- 20% Most accurate in high output states and less accurate in low output states
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Thermodilution curves – PA temperature vs time
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Vascular resistance In clinical practice Ohm’s law : Q = ∆ P / R is used to calculate resistance Systemic vascular resistance = AO mean - RA mean Q S Pulmonary vascular resistance = PA mean - LA mean QP pressures are in mmhg , flow in litres per min and resistance in Hybrid resistance unit or Wood’s unit expressed as mmhg / litre/ min Wood units can be converted to metric units by conversion factor 80 expressed as dynes.sec.cm -5 Vascular resistance is normalized for BSA giving a Resistance Index. SVRI = Ao(mean) – RA(mean) 80 ______________________ CI Where CI is Cardiac Index Thus SVRI = SVR x BSA
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NORMAL VALUES FOR VASCULAR RESISTANCE
Systemic vascular resistance dynes – sec – cm -5 Systemic vascular resistance index dynes – sec – cm-5 m2 Pulmonary vascular resistance dynes – sec – cm-5 Pulmonary vascular resistance index dynes – sec – cm-5 m2
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Thank you for your kind attention !
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