Water, strong ions, and weak ions

Water, strong ions, and weak ions
Gunjan Chawla MBBS DA
Gordon Drummond FRCA
Key points
The law of electrical
neutrality states that, in any
aqueous solution in
equilibrium, the sum of the
positive charges always
equals the sum of the
negative charges.
An acid or base is defined
as strong if it is fully
dissociated at the pH of
interest.
The term ‘acid– base balance’ was coined by
Henderson in the early 20th century. In his
work, CO2 was the centre of attention as it was
for a long time the only measurable quantity
relevant to acid –base status. Henderson applied
the law of mass action to the carbonic acid
equilibrium and we got the Henderson
equation:
½Hþ ¼ K0
½CO2 ½HCO
3
Strong ion difference (SID)
is the amount by which the
strong positive ions
(cations) are in excess of
the strong negative ions
(anions).
The role of respiratory control of PCO2 was
recognized and Hasselbach introduced this into
the equation and gave it a logarithmic form, the
Henderson–Hasselbach equation:
Weak acids and bases are
only partially dissociated in
the range of body pH.
½HCO
3
pH ¼ pK þ log
SCO2 PCO2
Acid – base balance can be
characterized quantitatively
in terms of three
independent variables: PCO2,
[SID], and total weak acid.
The dependent variables:
2
[HCO2
3 ], [HA], [A ],
2
22
[CO3 ], [OH ] and [Hþ]
or pH can be calculated
from these.
Gunjan Chawla MBBS DA
Senior House Officer
University Department of Anaesthetics
Critical Care and Pain Medicine
Royal Infirmary of Edinburgh
Edinburgh EH16 4SA
UK
Gordon Drummond FRCA
Senior Lecturer
University Department of Anaesthetics
Critical Care and Pain Medicine
Royal Infirmary of Edinburgh
Edinburgh EH16 4SA
UK
Tel: þ44 131 242 3134
Fax: þ44 131 242 3138
E-mail: [email protected]
(for correspondence)
108
The constant SCO2 (solubility factor ¼
0.03 mm litre21 mm Hg21 or 0.23 mm litre21
kPa21) allows conversion of PCO2 into [CO2].
Acid –base disturbances could now be
classified as respiratory or non-respiratory but
this had limitations. For pH to be determined
by CO2 and bicarbonate, these two had to be
independent of each other, which is not possible. In addition, the equation did not take
into account non-volatile weak acids present in
the body. To overcome these limitations,
Siggard-Anderson proposed PCO2-independent
indicators of acid –base disturbances. These
include standard bicarbonate, buffer base and
base excess/deficit. However, these approaches
do not take into account PCO2 and do not
differentiate between different causes of nonrespiratory acid –base disturbances.
In the 1980s, Stewart proposed a physicochemical approach to acid– base physiology.
The complex calculations involved in this
approach were not possible in the precomputer
era but are easily done today. He wrote of this
approach having ‘revolutionized our ability to
understand, predict and control what happens to
hydrogen ions in living systems’.
Definitions
‘Acid’ and ‘alkali’ are derived from Latin
(acidus ¼ sour) and Arabic (al qaliy ¼ ashes of
plant). Acids possess a sour taste in solution
and alkalis reverse their action in solution.
Using the simplest terminology, acidosis
denotes an excess addition of Hþ and alkalosis
an excess removal of Hþ.
The Arrhenius theory of acids and bases
was based on their dissociation into ions. Thus,
acids are defined as producers of hydrogen ions
and all bases produce hydroxyl ions. Lowry
and Bronsted gave this theory a more general
basis. They defined an acid as a molecule or
ion that can lose or donate a proton (a hydrogen ion is a single free proton released from a
hydrogen atom) and a base as a molecule or
ion that can accept a proton. Lewis further
extended this concept. He defined an acid as
any substance that accepts electrons and a base
as any substance able to donate electrons. Since
a Lowry–Bronsted base donates electrons to a
hydrogen ion, a Lowry–Bronsted base is also a
Lewis base. This concept usefully extends the
definitions of acid and base to include reactions
that do not involve hydrogen ions.
Stewart defined a solution as neutral if the
concentration of hydrogen ions was equal to
the concentration of hydroxyl ions, acidic if the
concentration of hydrogen ions was greater
than the concentration of hydroxyl ions and
basic if the concentration of hydroxyl ions was
greater than hydrogen ions. According to his
approach, an acid is a substance that increases
the [Hþ] of a solution and a base is a substance
that decreases it, relative to the hydroxyl ion
concentration. Electrolytes are substances that
dissociate into ions when dissolved in water.
Stewart classified these into strong and weak.
Strong electrolytes are always completely dissociated in solution and the resulting ions are
called strong ions. Weak electrolytes are substances that only partly dissociate into ions
when dissolved in water and yield weak ions.
The effects of strong and weak electrolytes on
acid –base balance are very different.
Electrolytes may yield (based on degree of
doi:10.1093/bjaceaccp/mkn017
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Water, strong ions, and weak ions
dissociation in solution): strong ions (complete dissociation),
2
e.g. Naþ, Kþ, Mg2þ, Ca2þ
SO22
4 , Cl , and weak ions (incomplete
,
dissociation), e.g. protein, phosphate, HCO2
3.
Stewart’s concept of acid– base: the
‘modern’ approach
According to this view, the acid– base state in different parts of the
body depends on: (i) water; (ii) strong ions; (iii) weak ions; and
(iv) solutions containing CO2 as indicated by the PCO2 of the solution. To understand this concept we have to keep the following
principles in mind:
1. The law of electroneutrality: this states that in aqueous solutions
in any compartment the sum of all the positive ions must equal
the sum of all the negatively charged ions.
2. The law of mass action: this law dictates the dissociation equilibria of incompletely dissociated substances.
3. The law of conservation of mass: the amount of a substance
remains constant unless it is added, removed, generated or
destroyed. The total concentration is the sum of the concentration of dissociated and undissociated forms.
Law of electrical neutrality
In any aqueous solution in equilibrium, the sum of the positive
charges always equals that of the negative charges. For instance, in
a solution of NaCl
½Naþ þ ½Hþ ¼ ½Cl þ ½OH This concept can be expressed graphically, using two columns:
one each for positive and negative charges, keeping them equal in
height. Gamble developed figures now called ‘Gamblegrams’ to
help express the composition of complex solutions such as plasma
(Fig. 1).
Fig. 1 Gamblegrams for NaCl solution, and after an increase in Naþ or
Cl2 ions in the solution.
Dissociation of water
Let us consider the water molecule. Water is formed by strong
covalent bonding between H and O and dissociates only very
slightly. The reaction: H2O $ Hþ þ OH2 is therefore far
to the left. At equilibrium, if we apply the law of mass action:
K [H2O] ¼ [Hþ] [OH2], the concentration of water [H2O] is
altered very minutely by dissociation; therefore, K [H2O] can be
taken as a constant known as K0 w (the ion product of water).
Therefore, [Hþ] [OH2] ¼ K0 w.
þ
2
To ensure electrical
pffiffiffiffiffiffiffiffi neutrality, [H ] ¼ [OH ] and 0 both
þ
2
0
[H ] and [OH ] ¼ K w. At 258C pure water has a K w of
1.008 10214 mol2 l23 and thus we can approximately state:
[Hþ] ¼ [OH2] ¼ 1027 Eq litre21. As activity increases with temperature, at 378C in solutions in the body, K0 w ¼ 4.4 10214 mol2 l23. Thus both [Hþ] and [OH2] are increased.
Pure water is always acid– base neutral, i.e. [Hþ] ¼ [OH2] but,
as described above, its hydrogen ion concentration varies considerably with temperature from pH 7.5 at 08C to pH 6.1 at 1008C. The
neutral pH (i.e. 7) occurs at 258C and at body temperature the
neutral pH is 6.8.
Water has a large dielectric constant. This means that molecules
containing strong ionic bonds dissociate to some extent in water.
Its own dissociation constant is small (10216 mEq litre21), i.e.
it dissociates to a very small extent. Thus the concentration of
hydrogen ions in body fluids is much lower than in water. The
extent of dissociation of water depends on temperature, concentration, ionic strength, and the presence of specific substances.
Water has a concentration of 55.3 M at 378C, which is around 400
times the concentration of any other substance in the body fluids
(Fig. 2). However, it is vital to realize that because water dissociates so little, the concentrations of hydrogen ions in body
fluids are very small. Hydrogen ion concentrations are measured in
NANO moles (nmol, 1029 mol) whereas important ions such as
sodium are present in concentrations nearly a million times greater
(mmol, 1023 mol) (Fig. 2). Figure 3 shows Gamblegrams for some
important body fluids.
Fig. 2 Relative concentrations of water and NaCl in the extracellular
fluids, and sodium and hydrogen ions in plasma.
Continuing Education in Anaesthesia, Critical Care & Pain j Volume 8 Number 3 2008
109
Water, strong ions, and weak ions
Fig. 3 Gamblegrams of ionic composition of body fluids.
Strong ions
Let us now explore the concept of strong ions. An acid or base is
defined as strong if it exists in a fully dissociated state at the pH of
interest. Consider the strong acid HX: the reaction HX ! Hþ þ
X2 is always far to the right. Similar conditions would apply for
the strong base BOH and the reaction BOH ! Bþ þ OH2. When
a known amount of HX or BOH is added to a solution, the
increase in X2 and Bþ is equal to the amounts added.
Strong ions are derived from compounds that dissociate completely in water. A strong ion is one that is always present in a
fully dissociated state. The predominant strong cations in blood are
Naþ, Kþ, Ca2þ, and Mg2þ, and Cl2 and SO22
4 . These relate to the
substances we think of as powerful acids and bases, such as sulphuric acid or sodium hydroxide. In a pure salt solution, NaCl
exists as equal amounts of Naþ and Cl2. Thus, the [Hþ] and pH of
the solution will remain unchanged upon addition of sodium chloride. Following the law of electrical neutrality: [Naþ] 2 [Cl2] þ
[Hþ] 2 [OH2] ¼ 0.
Addition of the strong acid HCl increases [Cl2] more than
[Naþ], thus [Hþ] increases to make up the difference and the solution becomes acidic. [OH2] must decrease because the dissociation equilibrium of water is constant and electrical neutrality
has to be maintained. On the other hand, addition of a strong
alkali NaOH increases [Naþ] more than [Cl2] and [OH2]
increases. By the law of mass action, and according to the dissociation constant of water, [Hþ] decreases so that [Hþ] [OH2]
is constant.
110
Fig 4. Strong ion differences.
Strong ion difference
SID (Fig. 4) indicates the amount by which the strong positive
ions (cations) are in excess of the strong negative ions (anions). It
is an indication of ‘unmeasured’ ions in the solution: SID þ
[Hþ] þ [OH2] ¼ 0 (law of electrical neutrality). SID . 0 implies
the presence of unmeasured anions, i.e. alkalosis. If the SID , 0,
this indicates the presence of unmeasured cations, i.e. acidosis. In
all biological fluids, SID is almost always positive. In mammalian
body fluids, it is approximately þ40 mEq litre21.
For
plasma:
SID ¼ [Naþ] þ [Kþ] þ [Mg2þ] þ [Ca2þ] 2
2
22
f[SO4 ] þ [Cl ]g but the simplification: SID ¼ [Naþ] þ [Kþ] 2
[Cl2] is generally sufficient, as these are the dominant ions.
Continuing Education in Anaesthesia, Critical Care & Pain j Volume 8 Number 3 2008
Water, strong ions, and weak ions
Within the cells: SID ¼ [Kþ] þ [Mg2þ] as the concentration of
other anions is very low and [Naþ] [Cl2].
SID as calculated above may be termed ‘inorganic’. However,
in diseases, organic strong ions such as lactate may make an
additional contribution to the SID. The SID for human fluids
can then be calculated as: SID ¼ [Naþ] þ [Kþ] þ [Mg2þ] þ
[Ca2þ] 2 f[lactate2] þ [Cl2]g. This is known as the apparent SID
or SIDa, as it does not take into account the role of weak acids
(buffers).
Figge et al. developed a formula for effective SID (SIDe),
which allowed the contribution of weak acids to be taken into
account. The strong ion gap (SIG) is the difference between apparent and effective SID and measures the contribution to SID of
unmeasured anions such as sulphate, ketoacids, pyruvate, acetate,
and gluconate. This is sometimes termed the ‘anion gap’.
Weak ions
Weak acids and bases are only partially dissociated in the range of
body pH. For a weak acid: HA $ Hþ þ A2. At equilibrium, the
flux in one direction is equal to that in the other, and the balance
may be affected by the other ions present. For a strong ion in solution, the ionized form X2 is unchanged whatever happens, but
for weak ions, only the total amount of A (Atot or HA þ A2) is
constant. The ratio [A2]/[HA] depends on the equilibrium constant
Ka. As [Hþ] increases, [A2] decreases and [HA] increases in
equal amounts. Following the law of mass action: [Hþ] ¼ Ka[HA]/
[A2] or pH ¼ pKa þ logf[A2]/[HA]g (Henderson–Hasselbach
equation). pKa can be defined as the pH at which the concentration
of a conjugate base equals that of the acid, the ‘midpoint’ of the
dissociation of the substance. pKa allows calculation of the degree
of dissociation at any pH.
The constraints of electrical neutrality imply that in a solution
containing both strong ions and weak ions, if something happens
to change the [H þ ], then the extent of the change will be less
than it would have been if strong ions alone had been present. This
brings us to the phenomenon of buffering. A buffer is a substance
which can bind or release Hþ in solution, and can maintain an
almost constant pH, despite addition of considerable amounts of
acid or base. The Henderson– Hasselbach equation is used to
describe the pH changes due to the addition of Hþ or OH2 to any
buffer system.
Principal buffers in body fluids are as follows:
(i) Blood:
H2CO3 $ Hþ þ HCO2
HProt $ Hþ þ Prot2;
3;
þ
2
HHb $ H þ Hb
(ii) Interstitial fluid: H2CO3 $ Hþ þ HCO2
3
(iii) Intracellular fluid: HProt $ Hþ þ Prot2
(iv) Kidneys:
H2CO3 $ Hþ þ HCO2
NH3 þ Hþ $ NH4;
3;
þ
2
2
HPO4 þ H $ H2PO4
Figge quantified the contribution of weak acids to SID as:
211
(i) Bicarbonate [HCO2
PCO2/102pH
3 ] ¼ 1000 2.46 10
Table 1 Clinical situations illustrating the interaction of SIG with weak acids
Metabolic change
SIG
Condition
Clinical scenario
Hyperalbuminaemia
Hypoalbuminaemia
Hyperphosphataemia
#
"
Acidosis
Alkalosis
Acidosis
ECF loss, cholera
Critically ill patients
Renal failure
(ii) Plasma protein, mainly albumin [Alb2] ¼ [Alb] (0.123 pH 2 0.631)
(iii) Phosphate [HPO22
4 ] ¼ [Phos] (0.309 pH 2 0.469)
22
(iv) SIDeff ¼ [HCO2
3 ] þ [Alb 2 ] þ [HPO4 ]
Weak acids cause a slight increase in the hydrogen ion concentration of the plasma. Therefore, a decrease in weak acids will
cause alkalosis, and an increase produces acidosis. Also note that
an increase in SID produces an increase in dissociated proteins and
an increase in PCO2 reduces dissociated protein.
Clinical situations illustrating the interaction of SIG with weak
acids are listed in Table 1.
Solutions containing carbon dioxide
We are already familiar with the CO2 –bicarbonate system. This is
an ‘open’ system capable of varying the total CO2 content within
wide limits. CO2 is present in the body in metabolic substrates, in
bone and as HCO2
3 in tissues. The ‘fixed’ stores cannot be
accessed but about 500 mmol is readily available. In the basal
state, a healthy adult produces at least 10 000 mmol of CO2 in
24 h. It is highly diffusible and completely equilibrates across
membranes. PCO2 is controlled by rapid changes in ventilation.
Thus, CO2 is the most mobile component and the CO2 –bicarbonate system a very powerful plasma buffer system.
The reaction involved is: H2CO3 $ Hþ þ HCO2
3 . Most buffers
are not free to leave the tissues and [Atot] is almost constant in any
particular compartment. However, CO2 is freely diffusible and
[CO2tot] (i.e. [H2CO3] þ [HCO2
3 ]) can vary considerably. CO2 dis22
solves in water producing H2CO3, HCO2
3 and CO3 . The concentrations of the dissolved CO2 and H2CO3 are directly proportional
þ
2
22
to the PCO2, but the concentrations of HCO2
3 and CO3 , H , OH
are also affected by changes in SID.
Summary
Stewart’s work has simplified our understanding of the mechanisms of conditions such as dilutional acidosis, concentrational alkalosis, hyperchloraemic acidosis, hypochloraemic alkalosis, and
hypoalbuminaemic alkalosis (Fig. 5). Using basic physicochemical
laws, such as the law of mass action, law of conservation of mass,
and the law of electrical neutrality, we can explain the acid– base
systems of the body. Acid– base balance can be understood quantitatively in terms of three independent variables:
PCO2, [SID] and total weak acid, i.e. [Atot] (usually protein and
phosphates) and their regulation by the lungs, kidneys, gut, and
Continuing Education in Anaesthesia, Critical Care & Pain j Volume 8 Number 3 2008
111
Water, strong ions, and weak ions
strong ions. Body fluids interact through membranes. Most membranes are impermeable to proteins under normal physiologic conditions so [Atot] interactions are significant only when disease
damages membranes.
Changes in respiration and circulation match the tissue production of carbon dioxide and control PCO2. These are responsible
for the acute alterations in acid– base disorders. Movement of Hþ
between solutions cannot affect the Hþ, only changes in the strong
ions can. Strong ions move freely in body fluids, across membranes. The kidneys and gut regulate their levels and thus are the
major determinants of SID in chronic acid –base disorders.
Further reading
Fig 5. Regulation of plasma composition according to Stewart’s concept.
2
22
liver. The dependent variables: [HCO2
3 ], [HA], [A ], [CO3 ],
2
þ
[OH ], and [H ] or pH can be calculated from these.
The pH and other dependent variables for any body fluid are
determined by the independent variables in that particular fluid
since hydrogen ions are affected by the other, more abundant,
112
Stewart PA. Modern quantitative acid-base chemistry. Canadian J Physiol
Pharmacol 1983; 61: 1444– 62
Rinaldi S, DeGaudio AR. Strong ion difference and strong anion gap: the
Stewart approach to acid base disturbances. Curr Anaesth Crit Care 2005;
16: 395–402
Gluck SL. Acid-base. Lancet 1998; 352: 474–79
Please see multiple choice questions 25 –29
Continuing Education in Anaesthesia, Critical Care & Pain j Volume 8 Number 3 2008