Formulas Flashcards

1
Q

Henderson Hasselbalch

A

determines how lipid soluble something is at a given pH if pKa is known.

Log (protonated concentration/unprotonated concentration) = pKa - pH

The higher the pKa, the stronger the acid (the more dissociated it is)

Acids are more water-soluble in alkaline solution
Bases are more water-soluble in acidic solution
Acids are more lipid-soluble in acidic solution
Bases are more lipid-soluble in basic solution

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2
Q

Shunt fraction (Berggren equation)

A

Qs/Qt = (CcO2 - CaO2) / (CcO2 - CvO2)

Qs/Qt = shunt fraction (shunt flow divided by total cardiac output)

CcO2 = pulmonary end-capillary O2 content, same as alveolar O2 content
the oxygen content of pulmonary endcapillary blood, and it is assumed that it is equal to CtO2 (A), the alveolar oxygen content. This assumption is based on a two-compartment model, where this compartment is perfectly oxygenated (i.e. the arterial and alveolar oxygen content is the same)

CaO2 = arterial O2 content
the oxygen content of systemic arterial blood, which will be lower than the content of “perfect” endcapillary blood because it is mixed with the relatively hypoxic Qs

CvO2 = mixed venous O2 content
the oxygencontent of mixed venous blood, is a known variable, and it is return to the lungs at a flow rate equal to the cardiac output, Qt

The estimated shunt fraction (Fshunte) can be calculated if an assumed value is substituted for CvO2 in the Berggren equation

“True” shunt can be identified if the subject is made to breathe 100% FiO2
- this decreases the contribution from V/Q scatter
- with 100% FiO2, the measured shunt fraction is the “true” intrapulmonary shunt
- This technique does not separate “true” shunt from anatomical shunt (contribution from thebesian veins and bronchial veins) or cardiac defects

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3
Q

Cardiac output

A

Cardiac output is definied as the volume of blood ejected by the heart per unit time. It is usually presented as
Stroke volume x heart rate in L/min

The determinants of cardiac output are:
- heart rate: a higher heart rate increases cardiac output as it multiplies by stroke volume; an excessively high heart rate decreases cardiac output by decreasing preload
- stroke volume, which in turn determined by preload, afterload, and contractility

Preload:
- increased preload leads to an increase in the stroke volume
- preload is determined by:
intrathoracic pressure
atrial contribution (atrial kick)
central venous pressure (RA pressure)
mean systemic filling pressure which depends on total venous blood volume and venous vascular compliance
compliance of the ventricle and pericardium
duration of ventricular diastole
end-systolic volume of the ventricle

Afterload:
- ventricular radius (end-diastolic volume)
- ventricular wall thickness
- ventricular transmural pressure
intrathoracic pressure
ventricular cavity pressure
ventricular outflow impedance and aortic input impedance
arterial resistance
- vessel radius
- blood viscosity
- length of the arterial tree
- inertia of the blood column
- influence of reflected pressure waves
- arterial compliance

Cardiac contractility:
- increased contractility improves stroke volume at any given preload or afterload value
- affected by: heart rate (bowditch effect), afterload (anrep effect), preload (frank-starling mechanism), cellular and extracellular calcium concentrations, temperature

Summary:
- stroke volume increases with increased preload, up to a plateau, beyond which it begins to decrease again
- stroke volume decreased with increased afterload, in a fairly linear fashion
- stroke volume increases with increased contractility, for any given preload and afterload value

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4
Q

Oxygen delivery

A

DO2 = Qt x CaO2

Where Qt is the cardiac output in L/min
CaO2 is the oxygen content of whole blood
the oxygen content of whole blood is the fraction of dissolved O2 and the product of Hb (g/L) x 1.39 In mL) multiplied by the saturation of hemoglobin

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5
Q

Systemic vascular resistance

A

SVR = (80 x (MAP - mean right atrial pressure) / cardiac output

SVR is the resistance (pressure drop) generated in blood flowing through the whole arterial circulation. Normally the pressure gradient is constant, and the flow is regulated by changes in vascular resistance.

Factors that affect SVR are the parameters of the Hagen-Poiseuille equation (length of the vessel, viscosity of the blood, radius of the vessel); arterial baroreflex control, peripheral and central chemoreceptors, pulmonary baroreceptors, hormones, temperature, intrinsic myogenic regulation, metabolic regulation, flow/shear associated regulation, conducted vasomotor responses, local cooling, immunological modulation by inflammatory mediators.

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6
Q

Respiratory quotient

A

The respiratory quotient, also known as the respiratory ratio (RQ), is defined as the volume of carbon dioxide released over the volume of oxygen absorbed during respiration. It is a dimensionless number used in a calculation for basal metabolic rate when estimated from carbon dioxide production to oxygen absorption.

RQ = CO2eliminated / O2consumed

RQ typically is reported as a known 0.8

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7
Q

CVP waveform

A

generally measured at the junction of the superior vena cava and the right atrium. This is most commonly done via a central venous catheter placed through the right internal jugular vein.

A normal CVP waveform contains five components. These components include three peaks (a, c, v) and two descents (x, y). All of these components correspond to various aspects of the cardiac cycle.

The first peak is the a-wave, which immediately follows the p wave of the ECG waveform. The a-wave is a pressure increase that is due to atrial contraction at end-diastole. Shortly after the a-wave there is a second peak, the c-wave. The c-wave immediately follows the r wave of the ECG waveform. This is a pressure increase due to tricuspid bulging into the atrium as a result of isovolumic ventricular contraction (IVC). Note that the a and c-waves are split by the r wave of the ECG waveform. This is because the a-wave always represents end-diastole and the c-wave represents early ventricular systole.

Following the c-wave is the first major descent in the CVP waveform, the x-descent. The x-descent is a drop in atrial pressure during ventricular systole caused by atrial relaxation. At the trough of the x-descent there is an increase in atrial pressure as the atrium begins to fill during late systole. This is called the v-wave. The v-wave corresponds to the end of the t wave in the ECG waveform. The final aspect of the CVP waveform is the y-descent, which is due to an atrial pressure drop as blood enters the ventricle during diastole.

Waveform Component: a-wave Phase of the cardiac cycle: end diastole Mechanical Event: atrial contraction

Waveform Component: c-wave Phase of the cardiac cycle: early systole Mechanical Event: Tricuspid bulging (IVC)

Waveform Component: v-wave Phase of the cardiac cycle: late sytole Mechanical Event: systolic filling of the atrium

Waveform Component: x-wave Phase of the cardiac cycle: mid systole Mechanical Event: atrial relaxation

Waveform Component: y-wave Phase of the cardiac cycle: early diastole Mechanical Event: early ventricular filling

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8
Q

CaO2

A

(arterial oxygen content) CaO2 = (SaO2 x Hb x 1.37) + (PaO2 mmHg x 0.003)

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9
Q

Bohr’s dead space equation

A

Physiological dead space can be measured using the Bohr-Enghoff method
- The Bohr equation can be used to determine physiological dead space from the difference between the exhaled CO2 and alveolar CO2 but the latter is hard to measure
The equation is Vd/Vt = (PACO2 - PECO2) / PACO2
- the Enghoff modification of the Bohr equation uses arterial CO2 instead of alveolar CO2 and is, therefore, easier to measure, but it is influenced by multiple factors such as: dead space, intrapulmonary shunt, diffusion impairment, V/Q heterogeneity

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10
Q

Pulmonary vascular resistance

A

Factors which influence pulmonary vascular resistance:
- Pulmonary blood flow:
- increased blood flow results in decreased pulmonary vascular resistance in order for pulmonary arterial pressure to remain stable
- distension of pulmonary capillaries
- recruitment of previously collapsed or narrowed capillaries

  • Lung volume
    • the relationship between lung volume and PVR is “U”-shaped
    • pulmonary vascular resistance is lowest at FRC
    • at low lung volumes, it increases due to the compression of larger vessels
    • at high lung volumes, it increases due to the compression of small vessels
  • hypoxic pulmonary vasoconstriction
    • a biphasic process (rapid immediate vasoconstriction over minutes, then a gradual increase in resistance over hours)
    • mainly due to the constriction of small distal pulmonary arteries
    • attenuated by: sepsis, pneumonia, hypothermia, iron infusion
  • metabolic and endocrine factors
    • catecholamines, arachidonic acid metabolites (thromboxane A2) and histamine increase PVR
    • hypercapnia and (independently) academia also increase pVR
    • alkalemia decreases PVR and suppresses hypoxic pulmonary vasoconstriction
    • hypothermia increases PVR and suppresses hypoxic pulmonary vasoconstriction
  • autonomic nervous system
    • alpha1 receptors: vasoconstriction
    • beta2 receptors: vasodilation
    • muscarinic M3 receptors: vasodilation
  • blood viscosity
    • PVR increases with increasing hematocrit
  • drug effects
    • pulmonary vasoconstrictor: adrenaline, noradrenaline, and adenosine
    • pulmonary vasodilators: nitric oxide, milrinone, levosimendan, sildenafil, vasopressin, bosantan/ambrisantan, prostacycline, and its analogs, calcium channel blockers and ACE-inhibitors
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11
Q

Boiling point

A

boiling point is defined as the temperature at which vapor pressure equals atmospheric pressure (760 mmHg). Boiling points are listed below (celsius):

Sevoflurane: 58.5
Desflurane: 22.8
Isoflurane: 48.5
Enflurane: 50.2
N2O: -88

(Desflurane: high volatility/moderate potency, requires the use of a special vaporizer for proper utilization of this gas. Desflurane vaporizers are heated to 39*C which increases the vapor

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12
Q

Heat of vaporization

A

In a closed container, molecules from a volatile liquid escape the liquid phase and become vapor. These gaseous molecules strike the wall of the container, exerting what’s known as vapor pressure. Vapor pressure is directly correlated with temperature. Increasing temperature will increase the ratio of gas:liquid molecules, thereby increasing vapor pressure.

Vapor pressure of volatile agents at 20 degrees C (mmHg):
- sevoflurane: 157
- desflurane: 669
- isoflurane: 238
- enflurane: 172
- halothane: 243
- N2O: 38,770

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13
Q

Saturated vapor pressure

A

Evaporation is the phenomenon by which molecules in the liquid phase (with high kinetic energy) escape from the surface of a liquid to enter the gas phase. Inside the vaporizer, molecules will enter the gas phase until the rate of vaporize molecules equals the rate of molecules returning to the liquid phase. This dynamic equilibrium is known as saturation. The pressure exerted by this gas is known as “saturated vapor pressure.” SVP increases in a non-linear fashion as the temperature of an anesthetic in the liquid phase increases and is independent of the barometric pressure. The SVP for all anesthetic gases is measured at 20*C and is a unique characteristic for each drug. (ex: iso SVP = 239 mmHg)

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14
Q

Specific heat

A

specific heat is the quantity of heat (calories) required to raise the temperature of a unit mass (grams) of a substance by 1*C. Heat must be supplied to the liquid anesthetic in the vaporizer to maintain the liquid’s temperature during the evaporation process, when heat is being lost.

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15
Q

Venous return

A

Venous return is the rate of blood flow into the heart form the veins. At a steady state, venous return and cardiac output are equal. Venous return can be expressed as:

VR = (MSFP - RAP) / VR where MSFP is mean systemic filling pressure and RAP is right atrial pressure and VR is the venous resistance

Factors which influence venous return include:
- factors which affect cardiac output: afterload, contractility
- factors which affect mean systemic filling pressure: total venous blood volume, venous smooth muscle tone
- factors which affect right atrial pressure: intrathoracic pressure (spontaneous v PPV), pericardial compliance, right atrial compliance, right atrial contractility, tricuspid valvular competence and resistance
- factors which affect venous resistance: mechanical factors (posture, intraabdominal pressure, skeletal muscle pump, obstruction to venous flow (pregnancy), hyperviscosity (polycythemia, hyperproteinemia)), neuroendocrine factors (autonomic tone, vasoactive drugs)

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16
Q

G protein coupled-receptors

A

The Gs and Gi pathways are important cell signaling pathways activated when a ligand binds to a G-protein coupled receptor, with a variety of downstream effects. These pathways both operate through the second messenger cAMP.

When a ligand binds to a Gs-coupled receptor, the Gs subunit is activated and stimulates the synthesis of cAMP. Conversely, if a Gi subunit is activated, it inhibits the synthesis of cAMP. cAMP in turn stimulates PKA, an important kinase enzyme with two downstream effects. First, PKA inhibits MLCK by phosphorylation, and second, PKA increases calcium levels in the heart by phosphorylation of calcium channels.

The Gq signaling pathway is a cell signaling pathway that starts with binding of a G-protein coupled receptor associated with a Gq protein subunit. This Gq subunit then stimulates the activation of PLC (phospholipase C). PLC is an enzyme that breaks down a membrane phospholipid (PIP2) into two intermediates, diacylglycerol (DAG) and inositol triphosphate (IP3). DAG goes on to activate another enzyme, protein kinase C (PKC). The other intermediate produced, IP3, induces the release of calcium ions from the sarcoplasmic or endoplasmic reticulum. This influx of calcium causes smooth muscle contraction.

17
Q

Events that occur during systole

A
  • Isovolumetric ventricular contraction
    • the beginning of this phase corresponds with the peak of the R wave
    • this corresponds to Phase 0 (rapid sodium influx) of the ventricular myocyte action potential
    • the ventricles begin to contract during this period
    • this contraction increases the ventricular chamber pressure and closes the mitral and tricuspid valves
    • as a result, there is a fixed ventricular volume during this contraction
  • early ejection
    - the contracting ventricles achieve a pressure high enough to open the aortic and pulmonic valves, and rapidly empty into the systemic and pulmonary circulations
    - this period corresponds to Phase 2 (plateau, rapid calcium influx) of the cardiac myocyte action potential
    - on the surface ECG, the end of this phase corresponds to the beginning of the T wave
  • Late ejection
    • this period begins when ventricular pressure starts to drop, and ends with the closure of the aortic pulmonic valves
    • the end of this period corresponds to the peak of the T wave on the surface ECG
    • this corresponds to Phase 3 (repolarisation) of the cardiac myocyte action potential
18
Q

Events during diastole

A
  • isovolumetric relaxation
    • the ventricles relax without any change in volume
    • the pressure drops until the tricuspid and mitral valves open
    • this period corresponds to the end of the T wave on the surface ECG, and the end of Phase 3 of the action potential
  • Early rapid diastolic filling
    - during this period the relaxing ventricles have pressure lower than atrial pressure, and they fill rapidly
    - 80% of the ventricular end-diastolic volume is achieved during this phase
    - coronary blood flow is maximal during this phase
  • late slow diastolic filling
    - ventricular and atrial pressures equilibrate and the atria act as passive conduits for ventricular filling
    - the end of this phase corresponds to the end of the P-wave on the surface ECG
  • atrial systole
    - the atria contract (right first, then left shortly after)
    - this increases the pressure in the ventricles up to the end-diastolic pressure, and adds about 20 mL of extra volume to the end-diastolic volume
    - these events start at the end of the P-wave on the surface ECG, and finish during the PR interval
    - the end of this phase corresponds to the peak of the R wave, or the Phase 0 (rapid sodium influx) of the ventricular myocyte action potential
19
Q

Systole

A

The period of chamber contraction and blood ejection which corresponds to the period between the QRS complex and the end of the T-wave. Additionally, the period between the closure of the mitral/tricuspid valves and the closure of the aortic/pulmonic valve

Phases
- isovolumetric ventricular contraction
- early ventricular systole
- late ventricular systole

20
Q

Diastole

A

The period of chamber relaxation and cardiac filling which corresponds to the period between the end of the T wave and the end of the PR interval. Additionally, the period during which the mitral valve/tricuspid valves are open.

Phases
- isovolumetric relaxation
- early ventricular diastole
- late ventricular diastole
- atrial systole

21
Q

The filling phase

A

Left ventricular systole.

The LA refills with pulmonary venous blood, taking advantage of the fact that the LV has decreased in volume. During this time, the LA fills with blood up to its maximum volume.

22
Q

Passive emptying phase

A

occurs when the mitral valve opens. Represents a period of rapid ventricular filling during early diastole

23
Q

Conduit phase

A

represents slow ventricular filling in late diastole and is the slow, boring period during which the LA does nothing active whatsoever (essentially a passive muscular tube through which pulmonary venous blood makes its way into the left ventricle)

24
Q

Active emptying phase

A

atrial contraction which empties a few extra mLs of blood into the left ventricle, contributing to its end-diastolic volume.

25
Q

Alveolar gas equation

A

This equation describes the concentration of gases in the alveolus.

PAO2 = (FiO2 x (Patmos - PH2O)) - (PaCO2 / RespQ)

PAO2 = partial pressure of alveolar oxygen
FiO2 = fraction of inspired oxygen, 0.21 in room air
Patmos = atmospheric pressure (760 mmHg at sea level)
PH2O = H2O vapour pressure in the alveolus - it’s usually 47 mmHg at 37C
PaCO2 = PaCO2 from the ABG
RespQ = respiratory quotient - usually 0.8

Rule of thumb: for every 10% increase in FiO2, the PAO2 will rise by about 71-72 mmHg

26
Q

Calculated osmolality

A

Osmolality is the number of osmoles of solute per kilogram of solvent. Osmolality depends on the mass of the solvent which is independent of temperature and pressure. Measurement of osmolaltiy is usually by freezing point depression, because it is also a colligative property and they are sufficiently related that one can be extrapolated from the other.

Example: calculated osmolality of normal saline is 300 (150 mOsm of Na and 150 mOsm of Cl) and it’s measured osmolality is 286.

Calculation of osmolality can never replace the measurement of osmolality.

Osmolality = deltaT / -1.86

deltaT = measured depression of the freezing point
-1.86 = cryoscopic constant for water ( basically that one mole of solute added to 1kg of water will depress its freezing point by 1.86*K)

27
Q

Reynolds Number

A

the ratio of inertial forces to viscous forces

Or

the ratio of gas density to gas viscosity.

Re = VDp / u

V = velocity of the gas flow
D = diameter of the tube
p = gas density
u = gas viscosity

This number describes whether the flow will be turbulent or laminar

Numbers under 2000 = flow is mainly laminar
Numbers 2000 - 4000 = flow is “transitional”, laminar turning to turbulent
Numbers >4000 = flow is mainly turbulent

28
Q

Laminar flow

A

Flow is proprotional to driving pressure, assuming the airway is straight and unbranced. The relationship of pressure gradient and flow rate is linear and is represented:
delta P = flow rate x resistance

Resistance is described by the classical Hagen-Poiseuille equation:

Resistance = (8 x length x viscosity) / pi x (radius)^4

29
Q

Turbulent flow

A

flow is proportional to the square root of driving dressure. As the pressure gradient increases, flow increases less (the relationship is not linear)

Resistance increases in proportion to flow rate and CANNOT be described using the traditional Hagen-Poiseuille equation. It is usually represented in terms of a pressure gradient:

Pressure gradient = K(flow)^n

K is an empirical constant which for the human respiratory tract, appears to be 0.24 (when the pressure gradient is expressed in kPa)
n is an exponent which is 1.0 for a purely laminar flow and 2.0 for a purely turbulent flow

the volume of gas moving through the tube is proportional to the volume of the tube

Density is the most important determinant of whether or not flow will be turbulent, all other things being equal.

30
Q

Rheobase

A

The threshold stimulus current for an active response with a long-duration pulse.

The minimum current required to depolarize a nerve given an infinite duration of stimulation

31
Q

Chronaxie

A

the pulse width at twice the rheobase threshold current

The duration of current required to depolarize a nerve to threshold when the current is two times the rheobase