Добавил:
kiopkiopkiop18@yandex.ru t.me/Prokururor I Вовсе не секретарь, но почту проверяю Опубликованный материал нарушает ваши авторские права? Сообщите нам.
Вуз: Предмет: Файл:

Ординатура / Хирургия / Библиотека им академика М.И. Перельмана / Книга_5769_Библиотеки_им_академика_М_И_Перельмана

.pdf
Скачиваний:
0
Добавлен:
30.08.2026
Размер:
65 Мб
Скачать
11
Echodynamics
General considerations
Hemodynamics is the study of blood flow with its related forces. e evaluation of hemo­dynamic parameters is crucial for the diagnosis and the rational therapy of the critically ill and the respiratory patients. Many instruments, with different complexity and methods, are employed for assessing such parameters.
anks to the application of Doppler technology, both transthoracic and transesophageal echography are useful bedside non invasive tools for providing hemodynamic information. is non invasive, ultrasound-guided assessment can be called “Echodynamics”
Doppler sonography provides excellent assessment of hemodynamics that compares favorably with more invasive and complex measurements. Monitoring using Pulmonary Artery Catheters (PAC), for long time considered as the gold standard, has not yet to improve survival and has many important limitations
Some information about the Doppler principle can be found in Chapter 1. Previous pages on echocardiography (Chapter 10) have already discussed the applications of cardiac ultrasound for a visual inspection and basic (focused) or intermediate hemodynamic interrogations (pres­sure determinations, stroke volume and diastolic function assessment).
is chapter briefly synthesizes the physical and methodological basis for the application of the Doppler sonography in the hemodynamically instable and in the critically ill patient For simplicity the discussion will cover only the use of transparietal ultrasound.
Finally, many important clinical consid­erations for an integrated approach to the critical patient will appear in the next chapter (Chapter 12, Integrated clinical ultrasound).
3,4,5
.
1,2
.
6,7,8
.
Pathophysiologic targets
Echocardiography is currently the only method that can provide real-time imaging of the heart at bedside. It represents the first line modality for estimating ventricular volumes, cardiac performance and the pericardial space (Fig. 1). ese arguments, that can be interpreted only qualitatively, are covered in the chapter on echocardiography in this book.
Preload assessment is important for the study of the hypotensive patient. It can be evaluated
Figure 1 – A simple visual assessment of the heart is determinant for detecting large devia­tion from normality. A: normal heart, B: enlarge­ment of the right ventricle. C: enlargement and remodeling of the left ventricle, and left atrial enlargement. D: pericardial effusion.
361
362 oracic ultrasound
by measuring left ventricular end diastolic volume or area. ese measures generally reveal small left ventricular cavities with a small hyperkinetic heart when the circulating volume is low. Otherwise, a small, collapsed inferior cava vein is the hallmark of the hypovolemic pa­tient (Fig. 2). e massively vasodilated patient without a severely impaired cardiac function, shows a small inferior cava vein and small end systolic left ventricular area and volume. is picture is characteristic of hyperdynamic septic and neurogenic shock (distributive shock).
Such observations can be suitably expanded to cover other important pathophysiologic targets. In fact, a comprehensive Doppler analysis enables sufficiently accurate quantitative assessment of stroke volume, cardiac output, ventricular filling pressure and systemic and pulmonary vascular resistances (Fig. 3).
Figure 2 – A: small telediastolic left ventricular area (parasternal short axis view) and small left telediastolic ventricular volume (four cambers view), with a small inferior cava vein (B), are hallmarks of volume depletion.
Figure 3 – Patient with severe heart failure. Synthetic morpho-functional evaluation. Many concordant information may be acquired by cardiac and hemodynamic ultrasound assessment. A: enlarged and remodeled left ventricle. Large left atrium. B: very low ejection fraction. C: wide/tight early (E) mitralic inflow wave (restrictive). D: small TDI E’ wave, and, as a result, high E/E’ ratio (high left ventricular filling pressure). E: high velocity mitral regurgitant flow. F: low stroke distance (VTI). From these two parameters, a high mitral regurgitant velocity/stroke distance ratio results (high systemic vascular resistances). Many other useful information may be acquired during pleural and lung ultrasound. A concordance between different morpho-functional data reinforces a clinical hypothesis and, above all, is basilar for monitoring and therapeutic purposes.
Echodynamics 363
A complete and quantitative sonographic assessment of the patient with heart failure, shock and sepsis requires an advanced ultrasound skill. Although this book mainly describes basic and intermediate ultrasound applications to the chest, a brief description of advanced ap­plications of Doppler sonography to hemodynamics is useful for a better comprehension of the previous and next pages.
Table 1 shows direct hemodynamic parameters and their echocardiographic correlates. Table 2 shows calculated (indirect) hemodynamic parameters. Table 3 summarizes the normal values of the most important cardiovascular measurements.
Table 1 – Echodynamic parameters
Hemodynamic parameter Echo correlate Comment
LVOT Velocity Time Integral (VTI) VTI Normally 18-22 cm
Stroke volume (ml) VTI ∙ LVOT area Accurate measure of LVOT
diameter is critical
Right atrial pressure (RAP) (mm/Hg) Inferior Caval vein
analysis
Left atrial pressure (LAP) (mm/Hg) SBP – 4(Vmr)
Ejection fraction (%) EDV-ESV / EDV Modified biplane Simpson’s rule
Pulmonary artery systolic pressure (mm/Hg)
Pulmonary artery diastolic pressure (mm/Hg)
Pulmonary capillary wedge pressure E/Em* Tissue Doppler analysis of
4(VTr)2 + RAP Continous Doppler of tricuspid
4(VPr)2 + RAP Continous Doppler of
2
Not valid in patients in positive pressure ventilation
Exclude patients with acute mitral regurgitation, prosthetic mitral valve, and LVOT obstruction
recommended
regurgitant jet velocity (VTr) is necessary
pulmonary valve regurgitant jet velocity (VPr) is necessary
mitral annulus is necessary. E/Em represents the ratio between the peak velocity of early transmitral flow (pulsed wave Doppler) and the speed of early tissue relaxation velocity, measured by Tissue Doppler Imaging.
Abbreviations: VTI: Velocity Time Integral; LVOT: Left ventricular outflow tract; HR: Heart rate; SBP: Systolic blood pressure; EDV: End diatolic volume; ESV: End systolic volume; Vmr: Mitral regurgitant velocity; VTr: Tricuspid regurgitant velocity; VPr: Pulmonary valve regurgitant velocity; E/Em: ratio between E and Em wave at Tissue Doppler Imaging A normal E/Em is less than 10. A ratio greater than 15 predicts a left ventricular filling pressure greater than 15 mm/Hg
364 oracic ultrasound
Table 2 – Indirect hemodynamic parameters
Hemodynamic parameter Equation
Body Surface Area (BSA) (m2) (Height in cm + Weight in Kg – 60)/100
Cardiac output (ml/min) HR X VTI X LVOT area
Cardiac index (ml/min ∙ m2) CO/BSA
Stroke volume index (ml/beat ∙ m2) SV/BSA
Systemic vascular resistence (SVR) (dyne ∙ sec/cm5) 80 (MAP – RAP) X1/CO
Pulmonary vascular resistence (PVR) (dyne ∙ sec/cm5) 80 (PAP – PCWP) X1/CO
Abbreviations: VTI: Velocity Time Integral; LVOT: Left ventricular outflow tract; HR: Heart rate; CO: Cardiac output; SV: Stroke volume; BSA: Body surface area; MAP: Mean arterial pressure; RAP: Right atrial pressure; PAP: Pulmonary artery pressure; PCWP: Pulmonary capillary wedge pressure
Table 3 – Normal values of the most important cardiovascular measurements
Cardiac output 4-7 L/min
Cardiac index 3.5-4 L/min
Stroke volume 42-52 ml
Stroke index 36-48 ml/m
2
Ejection fraction 55-75%
End diastolic LV area (4 ch) 33±8 cm
End systolic LV area (4 ch) 6±2 cm
End diastolic LV volume (4 ch) 60-95 ml/m
End systolic LV volume (4 ch) 18-32 ml/m
2
2
2
2
Right atrial pressure 1-8 mm/Hg
Pulmonary artery wedge pressure 5-15 mm/Hg
Right ventricular systolic pressure 15-25 mm/Hg
Right ventricular diastolic pressure 0-8 mm/Hg
Pulmonary artery systolic pressure 15-25 mm/Hg
Pulmonary artery diastolic pressure 8-15 mm/Hg
Systemic vascular resistance 1500-3000 dyn∙sec∙cm-5
or 18.7-37.5 WU
Pulmonary vascular resistance 100-250 dyn∙sec∙cm-5
or 1.25-3.12 WU
Echodynamics 365
Shock
Shock is the clinical expression of circulatory failure that results in inadequate cellular oxygen utilization9.
It results from four potential, and not necessarily exclusive, pathophysiological mechanisms: hypovolemia, cardiogenic factors, obstruction (pulmonary embolism, cardiac tamponade, tension pneumothorax), or distributive factors (sepsis, anaphylaxis, pancreatitis). In ICU, septic shock is the most common form of shock (62%), whereas obstructive shock is rela­tively rare (2%). Cardiogenic shock occurs in 16% of cases, hypovolemic shock in 16% and distributive shock in 2%.
e key for an etiologic diagnosis of shock is to identify the specific patterns in cardiocircula­tory failure and shock (Tab 4)10.
Table 4 – Cardiocirculatory patterns in shock
Type of shock CVP and LVFP Cardiac output Systemic vascular
resistance
Hypovolemic low low high low
Cardiogenic high low high low
Septic Hyperdynamic Hypodynamic
Obstructive High and low low high low
Neurogenic low low low low
Hypoadrenal high or low low low or normal low
high or low high or low
high low
low high
Venous O2 saturation
high low or high
From a practical point of view, hypovolemic shock is characteristic, because volume depletion is its main landmark. It is clearly expressed on heart and inferior cava vein (or internal jugular vein). e diagnosis of cardiogenic shock is relatively easy if the clinician is able to evalu­ate the systolic function of the heart and the stroke volume. Neurogenic and Hypoadrenal shock are relatively infrequent. Septic shock is usual in emergency and ICU and is the most heterogeneous shock in its hemodynamic features. Tipically, the early phase of septic shock is hyperdynamic, late phase is hypodynamic and it often shows an overlap with cardiogenic shock (see later, sepsis related cardiomyopathy).
erefore, an atypical, mixed, imperfect, hypovolemic/cardiogenic shock is often a septic shock. Finally, the diagnosis of obstructive shock in cardiac tamponade and in pulmonary embolism
is immediate. e first diagnosis is only inspective. e latter is clear if the clinician look at the right heart and at the lung11.
Physical considerations
ree main equations govern an echodynamic assessment:
• Flow equation
• Continuity equation
• Bernoulli equation
366 oracic ultrasound
According to the first equation, using the Doppler effect, the velocity of blood in an ana­tomic conduit (left ventricular outflow tract, just below the aortic valve) can be calculated. By integrating the blood velocities over time (velocity time integral - VTI), a stroke distance can be calculated. is is the distance (in cm) travelled by a column of blood during a fixed time (a single cardiac cycle). By multiplying this by the cross-sectional area (measured in B Mode) through which the column moves, a volume (SV) can be obtained according to equation 12,13 (Fig. 4).
SV = VTI · πr2
where SV represents the Stroke Volume. Finally, Cardiac Output (CO) is the product of SV and heart rate (HR):
CO=SV· HR
Figure 4 – Above: Assessment of the diameter of left ventricular outflow tract (LVOT) at the aortic annulus during systole, using a parasternal long axis view. Below: Velocity time integral (VTI) assessment using pulsed Doppler spectrum in four chambers view. The sample is placed 5 mm below the plane of the aortic valve. Stroke volume is the product of VTI and LVOT area.
Based on the principle of conservation of mass, the Continuity Equation states that the flow in one area must equal the flow in a second area, if there are no shunts between the two areas. is principle is used for the determination of aortic valve area during the assessment of aortic stenosis and for quantifying vascular stenosis. In aortic stenosis, the stroke volume within the left ventricular outflow tract must equal the stroke volume through the stenotic orifice. Because stroke volume is the product of cross sectional area and velocity time integral (VTI), the continuity equation can be arranged to yield:
Aortic valve area = LVOT area · VTIOT/VTIAS
Echodynamics 367
Where LVOT represents the cross sectional area of the left ventricular outflow tract, and VTIOT/ VTIAS the ratio between VTI of the outflow tract and VTI of the aortic stenosis jet (Fig. 5).
Figure 5 – Above: Pulsed Doppler sampling of the ejected flow through the left ventricular outflow tract in a normal subject, to calculate velocity-time integral (VTI). Below: Continuous wave Doppler envelope directed through the aortic valve in the same subject. VTI is calculated. The aortic valve area may be assessed according the continuity equation (in this normal case VTIOT/VTIAS is 0.88). Therefore aortic the valve area is LVTO areaX0.88.
e Bernoulli equation is very important in hemodynamics:
P+1/2ρV2 + ρgh=constant
it is derived from the Navier-Stokes equation in the case of inviscid and steady flow condi­tions. When applied to two cross-sections of a vessel it gives rise to the following equation
P1 P2 = 1/2ρ(V22 V12) + ρg(h2 − h1)
where P1 and P2 are the upstream and downstream pressures, respectively; V1 and V2 are the upstream and downstream velocities, respectively; ρ is blood density and can be supposed to be 1.06 gr/cm3; g is the gravitational acceleration (9.8 m/sec2); h1 and h2 are the upstream and downstream heights of the vessel, respectively. However, in practical clinical terms, the difference between h1 and h2 is minimal, and therefore can be ignored (the addendum ρg(h2-h1)= 0). Also, as the blood flows through a narrowed orifice, the proximal velocity V1 is much smaller compared to the velocity downstream V2. Because the equation involves the square of both velocities, V1 has little impact in most cases. erefore, for routine clinical applications, a pressure gradient is estimated only by measuring the downstream velocity V2.
P1 P2 = 1/2V2
368 oracic ultrasound
Moreover, if the pressure gradient ∆P is converted from Pascal units to mmHg, the practical and well known equation is obtained
∆P = 4V2
where V is the Doppler derived velocity in m/sec and ∆P represents the peak instantaneous or maximal pressure gradient in mm Hg.
Bernoulli’s equation measures pressure difference (or gradient) between chambers and not the absolute pressure within them. Calculation of the absolute pressure within a particular chamber from the pressure gradient, obtained through Bernoulli’s equation, requires knowl­edge of a reference pressure and other assumptions.
A widespread use of Bernoulli’s equation is for the estimation of right ventricular and pul­monary artery systolic pressures. In this setting, the peak tricuspid regurgitant jet velocity, obtained on continuous wave Doppler, is used to calculate peak pressure gradient between the RV and RA during systole. Right ventricular systolic pressure (RVSP) is then calculated by adding estimated right atrial pressure, calculated by the inferior cava volume and collapsibility, to the measured gradient. Pulmonary artery systolic pressure (PASP) can be deduced from this, because it would be equal to RVSP in the absence of pulmonary stenosis. In a similar way pressure gradients can be calculated through aortic and mitral valves, and left atrial and ventricular pressures consequently assessed.
A list of clinical applications of Bernoulli’s equation is provided in Table 5.
Table 5 – Clinical applications of Bernoulli’s equation
Clinical applications Utility
Peak velocity across a valve Valvular stenosis maximal gradient (mm/Hg)
Left ventricular outflow tract contour and peak velocity
Mitral regurgitant velocity Left atrial pressure
Tricuspid regurgitant jet velocity Right ventricle systolic pressure, Pulmonary artery
Dynamic outflow tract obstruction, hypertrophic obstructive cardiomyopathy
systolic pressure (in absence of pulmonary stenosis), Pulmonary artery diastolic pressure
Clinical implications
e most common use of the Bernoulli’s equation is to evaluate the severity of a valvular stenosis and to assess transvalvular pressure gradients. For simplicity, we will discuss only the mitral and aortic valves stenosis.
Aortic stenosis (AS) is the most frequent valvular heart disease. In a patient with chest pain, syncope, pulmonary edema, arrhythmia, and unexplained hypotension or shock, a rapid diagnosis of AS is crucial.
e development of AS-related symptoms marks a critical point of disease progression in subjects with aortic stenosis for which there is no specific medical therapy.
Mitral stenosis is relatively less frequent and shows a relatively good prognosis, and surgery is indicated only when symptoms appear, but this observation is being reconsidered based on the risk of systemic embolization and the recurrences of pulmonary edema.
Echodynamics 369
On the other hand, valvular regurgitation14, which may be diagnosed only by visual and color Doppler inspection (Fig. 6) (Tab. 6), is important in emergency and critical care medicine if related to acute valvular or subvalvular disruption, infective endocarditis or to acute aortic syndrome (in the case of acute aortic regurgitation).
Figure 6 – A: mitral regurgitation. B: tricuspid regurgitation. C: severe mitral regurgitation. D: aortic regurgitation.
Table 6 – Inspective and color flow parameters for valvular regurgitation severity
Valve Modality Parameter Criteria for severe Comment
Aortic Color Doppler Jet area >60% LVOT area Instrument
Color Doppler Jet height >60% LVOT height
2D echocardiography LVED dimension > 7 cm Non specific,
2D echocardiography LVES dimension > 4.5 cm
Mitral 2D echocardiography LV size From large to very
2D echocardiography LA size
Color Doppler Jet area > 50% LA < 15% LA: mild
Abbreviations: LVOT: Left ventricular outflow tract; LVED: Left ventricular end diastolic; LVES: Left ventricular end systolic; LV: Left ventricle; LA: Left atrium
large
dependent, eccentric jet, temporal variations
affected by multiple factors
Normal size in mild and grade II severity
15-30% LA: grade II 35-50% LA: grade III
Valvular aortic stenosis
Normally, the aortic annulus is large between 1.4 and 2.6 cm. Aortic cusps show a systolic excursion of 90°, arranging themselves parallel to the aortic wall. e normal, non-stenotic aortic valve has an opening area of 3-4 cm2, which is equivalent to the area of the left ven­tricular outflow tract (LVOT) or aortic annulus.