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A. Loudness processing in acoustic nerve (at constant sound frequency)

of Acoustic Information

 

Quiet

Louder

Even louder

 

 

 

 

Cochlea

Acoustic

Action potentials

 

Processing

nerve fibers

 

 

 

 

 

B. Binaural hearing: lag time and latency differences

 

Central

 

Sound velocity

Sound pressure

Pressure

 

 

 

Lag time

 

difference

12.30

 

 

 

 

 

 

 

 

Central

 

 

Plate

 

excitation

 

 

 

 

Latency time

 

 

 

 

for nerve

 

 

 

Nearer ear

conduction

 

 

 

Difference

 

 

 

 

 

 

 

 

in latency

 

 

 

Averted ear

 

Soundpressure

 

 

Difference in sound pressure

 

 

 

 

C. Cochlear potentials and electrolyte

D. Afferent auditory pathway

 

 

distribution

(See text on p. 366)

 

 

 

10

 

 

 

 

 

 

 

Primary

 

 

 

 

 

 

 

 

 

auditory

 

 

 

–70

 

 

 

 

 

cortex

 

 

 

 

 

 

 

 

 

 

 

 

 

Endolymph

Perilymph

MGB

 

9

8

8

9

 

 

 

 

 

 

mV

 

 

Superior

 

 

 

Na+

 

 

 

7

7

 

 

Stria

K+

Inferior

 

 

 

 

+

quadrigeminal bodies

 

 

 

 

 

vascularis

K Na+

 

Nucl. of

 

6

 

 

6

 

 

 

 

lateral lemniscus

 

 

 

 

 

+80 to +110

 

K+

Nucl.

 

 

 

 

 

 

 

 

 

accessorius

 

 

 

 

 

 

 

 

 

Superior

 

4

5

 

 

 

 

 

Na+

olive

 

 

 

 

–70 (External HC)

Nucl. cochlearis

 

3

 

 

 

 

 

dorsalis

 

 

 

 

 

–40 (Internal HC)

 

 

ventralis

1

2

 

 

 

 

 

 

 

 

 

 

 

 

 

 

0

 

 

 

 

 

 

 

 

 

 

 

Cochlea

 

 

 

 

De-

369

 

 

 

 

 

 

 

cussation

 

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All rights reserved. Usage subject to terms and conditions of license.

Voice and Speech

 

The human voice primarily functions as a

 

means of communication, the performance of

 

which is based on the human capacity of hear-

 

ing (!p. 363 B). As in wind instruments, the

Senses

body contains a wind space (trachea, bronchi,

etc.). Air is driven through the space between

space (passages above the glottis), which sets

and

the vocal cords (rima glottidis) into the air

the vocal cords into vibration. The air space

 

System

consists of the throat and oronasal cavities

(!A). The range of the human voice is so im-

 

 

mense because of the large variety of muscles

Nervous

that function to modulate the intensity of the

damental tone) and size/shape of the air space

 

airstream (loudness), tension of the vocal

 

cords, shape/width of the vocal cords (fun-

Central

(timbre, formants) of each individual.

adjust the vocal cords and rima glottidis. A

 

Joints and muscles of the larynx function to

12

stream of air opens and closes the rima glot-

tidis and sets off the rolling movement of the

 

 

vocal cords (!B). When a deep tone is pro-

 

duced, the fissure of the glottis remains closed

 

longer than it opens (ratio of 5 : 1 at 100 Hz).

 

This ratio drops to 1.4 : 1 in higher tones

 

(400 Hz). The rima glottis remains open when

 

whispering or singing falsetto (!C, blue).

 

Motor signals originate in the motosensory

 

cortex (!p. 325 C/B, tongue/throat) and are

 

conducted via the vagus nerve to the larynx.

 

Sensory impulses responsible for voice pro-

 

duction and the cough reflex are also con-

 

ducted by the vagus nerve. Sensory fibers from

 

the mucosa and muscle spindles of the larynx

 

(!p. 316) continuously transmit information

 

on the position and tension of the vocal cords

 

to the CNS. These reflexes and the close con-

 

nection of the auditory pathway with bulbar

 

and cortical motor speech centers are impor-

 

tant for fine adjustment of the voice.

 

Vowels (!D). Although their fundamental frequen-

 

cies are similar (100–130 Hz), spoken vowels can be

 

distinguished by their characteristic overtones (for-

 

mants). Different formants are produced by modify-

 

ing the shape of oral tract, i.e., mouth and lips (!D).

 

The three primary vowels [a:], [i:], [u:] make up the

 

vowel triangle; [œ:], [!:], [ø:], [y:], [æ:], and [!] are

370

intermediates (!D).

The phonetic notation used here is that of the In-

 

ternational Phonetic Society. The symbols mentioned

here are as follows: [a:] as in glass; [i:] as in beat; [u:] as in food; [œ:] as in French peur; [!:] as in bought; [ø:] as in French peu or in German hören; [y:] as in French menu or in German trüb; [æ:] as in bad; [!:] as in head.

Consonants are described according to their site of articulation as labial (lips, teeth), e.g. P/B/W/F/M; dental (teeth, tongue), e.g. D/T/S/M; lingual (tongue, front of soft palate), e.g. L; guttural (back of tongue and soft palate), e.g. G/K. Consonants can be also defined according to their manner of articulation, e.g., plosives or stop consonants (P/B/T/D/K/G), fricatives

(F/V/W/S/Ch) and vibratives (R).

The frequency range of the voice, including formants, is roughly 40–2000 Hz. Sibilants like /s/ and /z/ have higher-frequency fractions. Individuals suffering from presbyacusis or other forms of sensorineural hearing loss are often unable to hear sibilants, making it impossible for them to distinguish between words like “bad” and “bass.” The tonal range (fundamental tone, !C) of the spoken voice is roughly one octave; that of the singing voice is roughly two octaves in untrained singers, and over three octaves in trained singers.

Language (see also p. 336). The main components of verbal communication are (a) auditory signal processing (!p. 368), (b) central speech production and (c) execution of motor speech function. The centers for speech comprehension are mainly located in the posterior part of area 22, i.e., Wernicke’s area (!p. 311 E). Lesions of it result in a loss of language comprehension capacity (sensory aphasia). The patient will speak fluently yet often incomprehensibly, but does not notice it because of his/her disturbed comprehension capacity. The patient is also unable to understand complicated sentences or written words. The centers for speech production are mainly located in areas 44 and 45, i.e., Broca’s area (!p. 311 E). It controlls the primary speech centers of the sensorimotor cortex.

Lesions of this and other cortical centers (e.g., gyrus angularis) result in disorders of speech production (motor aphasia). The typical patient is either completely unable to speak or can only express himself in telegraphic style. Another form of aphasia is characterized by the forgetfulness of words (anomic or amnestic aphasia). Lesions of executive motor centers (corticobulbar tracts, cerebellum) cause various speech disorders. Auditory feedback is extremely important for speech. When a person goes deaf, speech deteriorates to an appreciable extent. Children born deaf do not learn to speak.

Despopoulos, Color Atlas of Physiology © 2003 Thieme

All rights reserved. Usage subject to terms and conditions of license.

A. Larynx (cross-section)

B. Motion of vocal cords

 

 

To oropharyngeal tract

To

 

 

 

 

esophagus

 

 

 

Rima glottidis

1

2

3

4

 

 

 

 

(After Smith)

Vocal cords

 

 

 

To trachea

 

1– 4

 

 

(wind space)

 

 

(After Paulsen)

 

 

 

 

C. Vocal range and singing range

 

 

 

 

 

 

 

 

 

Fundamental tones of speech

 

 

 

 

 

 

 

Male

 

Female

 

 

 

 

Note

 

E

H

e

h

e1

h1

e2

h2

e3

Frequency

81.5

122

163

244

326

488

652

977

1304

 

(Hz)

 

 

 

 

 

 

 

 

 

 

range

Bass

 

 

 

 

 

 

 

 

 

Tenor

 

 

 

 

 

 

 

 

 

Singing

Alto

 

 

 

 

 

 

 

 

 

Soprano

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

Chest tones

 

Middle tones

 

Head tones

Extremes

 

 

 

 

 

 

 

 

 

(After Stockhausen-Spiess)

D. Vowel production

 

 

a:

A

 

 

 

 

 

oe

ae

 

:c

o

e

 

 

a:

 

 

 

u:

 

y

i:

 

Vocal triangle

 

U I

u: i:

Hz 100

1000

5000

100

1000

5000

100

1000

5000

Fundamental

Formant range

 

 

 

 

 

 

tone

 

 

 

 

(After Grützner and Freystedt)

 

 

 

 

 

Plate 12.31 Voice and Speech

371

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13 Appendix

Dimensions and Units

Physiology is the science of life processes and bodily functions. Since they are largely based on physical and chemical laws, the investigation, understanding, assessment, and manipulation of these functions is inseparably linked to the measurement of physical, chemical, and other parameters, such as blood pressure, hearing capacity, blood pH, and cardiac output. The units for measurement of these parameters are listed in this section. We have given preference to the international system of SI units (Système International d’Unités) for uniformity and ease of calculation. Non-SI units will be marked with an asterisk. Conversion factors for older units are also listed. Complicated or less common physiological units (e.g., wall tension, flow resistance, compliance) are generally explained in the book as they appear. However, some especially important terms that are often (not always correctly) used in physiology will be explained in the Appendix, e.g., concentration, activity, osmolality, osmotic pressure, oncotic pressure, and pH.

The seven base units of the SI system.

Unit

Symbol

Dimension

 

 

 

Meter

m

length

Kilogram

kg

mass

Second

s

time

Mole

mol

amount of substance

Ampere

A

electric current

Kelvin

K

temperature (absolute)

Candela

cd

luminous intensity

 

 

 

The base units are precisely defined autonomous units. All other units are derived by multiplying or dividing base units and are therefore referred to as derived units, e.g.:

Area (length · length): m · m = m2

Velocity (length/time): m/s = m · s–1.

If the new unit becomes too complicated, it is given a new name and a corresponding symbol, e.g., force = m · kg · s–2 = N (! Table 1).

Fractions and Multiples of Units

Prefixes are used to denote decimal multiples and fractions of a unit since it is both tedious and confusing to write large numbers. We generally write 10 kg (kilograms) and 10 µg (micrograms) instead of 10 000 g and 0.00001 g, for example. The prefixes, which are usually varied in 1000-unit increments, and the corresponding symbols and conversion factors are listed in Table 2. Prefixes are used with base units and the units derived from them (! Table 1), e.g., 103 Pa = 1 kPa. Decimal increments are used in some cases (e.g., da, h, d, and c; ! Table 2). Time is given in conventional nondecimal units, i.e., seconds (s), minutes (min), hours (h), and days (d).

Length, Area, Volume

The meter (m) is the SI unit of length. Other units of length have also been used.

Examples:

1 ångström (Å) = 10-10 m = 0.1 nm 1 micron ( µ) = 10-6 m = 1 µm

1 millimicron (mµ) = 10-9 m = 1 nm

American and British units of length: 1 inch = 0.0254 m = 25.4 mm

1 foot = 0.3048 m

1 yard = 3 feet = 0.9144 m

1 (statute) mile = 1609.344 m !1.61 km

1 nautical mile = 1.853 km

The square meter (m2) is the derived SI unit of area, and the cubic meter (m3) is the corresponding unit of volume. When denoting the fractions or multiples of these units with prefixes (Table 2), please note that there are some peculiarities.

Examples:

1 m = 103 mm, but

1 mm2 = 106 mm2, and 1 m3 = 109 mm3

The liter (L or l)* is often used as a unit of volume for liquids and gases:

1 L = 10–3 m3 = 1 dm3 1 mL = 10–6 m3 = 1 cm3

1 µL = 10–9 m3 = 1 mm3.

372

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Table 1 Derived units based on SI base units m, kg, s, cd, and A

Coulomb

C

electrical charge

s · A

 

 

 

 

Farad

F

electrical capacitance

C · V–1 = m–2 · kg–1 · s4 · A2

Hertz

Hz

frequency

s–1

Joule

J

heat, energy, work

N · m = m2 · kg · s–2

Lumen

lm

light flux

cd · sr

 

 

 

 

Lux

lx

light intensity

Im · m–2 = cd · sr · m–2

Newton

N

force

m · kg · s–2

Ohm

Ω

electrical resistance

V · A–1 = m2 · kg · s-3 · A–2

Pascal

P

pressure

N · m–2 = m–1 · kg · s–2

Siemens

S

conductivity

Ω–1 = m–2 · kg–1 · s3 · A2

Steradian

sr

measure of solid angle1

1 (m2 · m–2)

Tesla

T

magnetic flux density

Wb · m–2 = kg · s–2 · A–1

Volt

V

electric potential

W · A–1 = m2 · kg · s-3 · A–1

Watt

W

electric power

J · s–1 = m2 · kg · s-3

Weber

Wb

magnetic flux

V · s = m2 · kg · s–2 · A–1

1The solid angle of a sphere is defined as the angle subtended at the center of a sphere by an area (A) on its surface times the square of its radius (r2). A steradian (sr) is the solid angle for which r = 1 m and A = 1 m2, that is, 1 sr = 1 m2/m–2.

Table 2 Prefixes for fractions and multiples of units of measure

Prefix

Symbol

Factor

Prefix

Symbol

Factor

 

 

 

 

 

 

deca-

da

101

deci-

d

10–1

hecto-

h

102

centi-

c

10–2

kilo-

k

103

milli-

m

10–3

mega-

M

106

micro-

µ

10–6

giga-

G

109

nano-

n

10–9

tera-

T

1012

pico-

p

10–12

peta-

P

1015

femto-

f

10–15

exa-

E

1018

atto-

a

10–18

Dimensions and Units

373

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13 Appendix

374

Conversion of American and British volume units into SI units:

1 fluid ounce (USA) = 29.57 mL

1 fluid ounce (UK) = 28.47 mL

1 liquid gallon (USA) = 3.785 L

1 liquid gallon (UK) = 4.546 L

1 pint (USA) = 473.12 mL

1 pint (UK) = 569.4 mL

Velocity, Frequency, Acceleration

Velocity is the distance traveled per unit time (m · s–1). This is an expression of linear velocity, whereas “volume velocity” is used to express the volume flow per unit time. The latter is expressed as L · s–1 or m3 · s–1.

Frequency is used to describe how often a periodic event (pulse, breathing, etc.) occurs per unit time. The SI unit of frequency is s–1 or hertz (Hz). min–1 is also commonly used:

min–1 = 1/60 Hz !0.0167 Hz.

Acceleration, or velocity change per unit time, is expressed in m · s–1 · s–1 = m · s–2. Since deceleration is equivalent to negative acceleration, acceleration and deceleration can both be expressed in m · s–2.

Force and Pressure

Force equals mass times acceleration. Weight is a special case of force as weight equals mass times acceleration of gravity. Since the unit of mass is kg and that of acceleration m · s–2, force is expressed in m · kg · s–2 = newton (N). The older units of force are converted into N as follows:

1 dyn = 10-5 N = 10 µN

1 pond = 9.8 · 10-3 N = 9.8 mN.

Pressure equals force per unit area, so the SI unit of pressure is N · m–2 = pascal (Pa). However, the pressure of bodily fluids is usually measured in mm Hg. This unit and other units are converted into SI units as follows:

1 mm H2O !9.8 Pa

1 cm H2O !98 Pa

1 mm Hg = 133.3 Pa = 0.1333 kPa

1 torr = 133.3 Pa = 0.1333 kPa

1 technical atmosphere (at) !98.067 kPa

1 physical atmosphere (atm) = 101.324 kPa

1 dyne · cm–2 = 0.1 Pa

1 bar = 100 kPa.

Work, Energy, Heat, Power

Work equals force times distance, N · m = J (joule), or pressure times volume, (N · m–2) · m3

= J. Energy and heat are also expressed in J. Other units of work, heat, and energy are

converted into J as follows: 1 erg = 10-7 J = 0.1 µJ

1 cal !4.185 J

1 kcal !4185 J = 4.185 kJ

1 Ws = 1 J

1 kWh = 3.6 · 106 J = 3.6 MJ.

Power equals work per unit time and is expressed in watts (W), where W = J · s–1. Heat flow is also expressed in W. Other units of power are converted into W as follows:

1 erg · s–1 = 10–7 W = 0.1 µW

1 cal · h–1 = 1.163 · 10-3 W = 1.163 mW

1 metric horse power (hp) = 735.5 W =

0.7355 kW.

Mass, Amount of Substance

The base unit of mass is the kilogram (kg), which is unusual insofar as the base unit bears the prefix “kilo”. Moreover, 1000 kg is defined as a metric ton* instead of as a megagram. Weight is the product of mass and gravity (see above), but weight scales are usually calibrated in units of mass (g, kg).

British and American units of mass are converted into SI units as follows.

Avoirdupois weight:

1 ounce (oz.) = 28.35 g

1 pound (lb.) = 453.6 g

Apothecary’s and troy weight:

1 ounce = 31.1 g

1 pound = 373.2 g.

The mass of a molecule or an atom (molecular or atomic mass) is often expressed in daltons (Da)*. 1 Da = 1/12 the mass of a 12C atom, equivalent to 1 kg/Avogadro’s constant = 1 kg/ (6.022 · 1023):

1 Da = 1.66 · 10-27 kg

1000 Da = 1 kDa.

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The relative molecular mass (Mr), or molecular “weight”, is the molecular mass of a substance divided by 1/12 the mass of a 12C atom. Since Mr is a ratio, it is a dimensionless unit.

The amount of substance, or mole (mol), is related to mass. One mole of substance contains as many elementary particles (atoms, molecules, ions) as 12 g of the nuclide of a 12C atom = 6.022 · 1023 particles. The conversion factor between moles and mass is therefore: 1 mole equals the mass of substance (in grams) corresponding to the relative molecular, ionic, or atomic mass of the substance. In other words, it expresses how much higher the mass of the atom, molecule, or ion is than 1/12 that of a 12C atom.

Examples:

Relative molecular mass of H2O: 18

!1 mol H2O = 18 g H2O.

Relative atomic mass of Na+: 23

!1 mol Na+ = 23 g Na+.

Relative molecular mass of CaCl2:

=40 + (2 · 35.5) = 111

!1 mol CaCl2 = 111 g CaCl2.

(CaCl2 contains 2 mol Cland 1 mol Ca2+.)

The equivalent mass is calculated as moles divided by the valency of the ion in question and expressed in equivalents (Eq)*. The mole and equivalent values of monovalent ions are identical:

1 Eq Na+ = 1/1 mol Na+.

For bivalent ions, equivalent = 1/2 mole:

1 Eq Ca2+ = 1/2 mole Ca2+ or 1 mole Ca2+ = 2 Eq Ca2+.

The osmole (Osm) is also derived from the mole (see below).

Electrical Units

Electrical current is the flow of charged particles, e.g., of electrons through a wire or of ions through a cell membrane. The number of particles moving per unit time is measured in amperes (A). Electrical current cannot occur unless there is an electrical potential difference, in short also called potential, voltage, or tension. Batteries and generators are used to create such potentials. Most electrical potentials in the body are generated by ionic flow (! p. 32). The volt (V) is the SI unit of electrical potential (! Table 1).

How much electrical current flows at a given potential depends on the amount of electrical resistance, as is described in Ohm’s law

(voltage = current · resistance). The unit of electrical resistance is ohm (Ω) (! Table 1). Conductivity is the reciprocal of resistance (1/Ω) and is expressed in siemens (S), where S = Ω–1. In physiology, resistance is related to the membrane surface area (Ω · m2). The reciprocal of this defines the membrane conductance to a given ion: Ω–1 · m–2 = S · m–2 (! p. 32).

Electrical work or energy is expressed in joules (J) or watt seconds (Ws), whereas electrical power is expressed in watts (W).

The electrical capacitance of a capacitor, e.g., a cell membrane, is the ratio of charge (C) to potential (V); it is expressed in farads (F) (! Table 1).

Direct current (DC) always flows in one direction, whereas the direction of flow of alternating current (AC) constantly changes. The frequency of one cycle of change per unit time is expressed in hertz (Hz). Mains current is generally 60 Hz in the USA and 50 Hz in Europe.

Temperature

Kelvin (K) is the SI unit of temperature. The lowest possible temperature is 0 K, or absolute zero. The Celsius or centigrade scale is derived from the Kelvin scale. The temperature in degrees Celsius (!C) can easily be converted into K:

!C = K - 273.15.

In the USA, temperatures are normally given in degrees Fahrenheit (!F). Conversions between Fahrenheit and Celsius are made as follows:

!F = (9/5 · !C) + 32

!C = (!F - 32) · 5/9.

Some important Kelvin, Celsius, and Fahrenheit temperature equivalents:

 

K

!C

!F

 

 

 

 

Freezing point of water

+ 273

0!

+ 32!

 

 

 

 

Room temperature

293–

20!–

68!– 77!

 

298

25!

 

 

 

 

 

Body core temperature

310

37!

98.6!

 

 

 

 

Fever

311–

38!–

100!–

 

315

42!

108!

 

 

 

 

Boiling point of water

373

100!

212!

(at sea level)

 

 

 

 

 

 

 

Dimensions and Units

375

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Concentrations, Fractions, Activity

The word concentration is used to describe many different relationships in physiology and medicine. Concentration of a substance X is often abbreviated as [X]. Some concentrations are listed below:

Mass concentration, or the mass of a substance per unit volume (e.g., g/L = kg/m3)

Molar concentration, or the amount of a substance per unit volume (e.g., mol/L)

Molal concentration, or the amount of substance per unit mass of solvent (e.g., mol/ kg H2O).

 

The SI unit of mass concentration is g/L (kg/m3,

 

mg/L, etc.). The conversion factors for older

 

units are listed below:

Appendix

1 g/100 mL = 10 g/L

1 g% = 10 g/L

 

 

1 % (w/v) = 10 g/L

 

1 g‰ = 1 g/L

13

1 mg% = 10 mg/L

1 mg/100 mL = 10 mg/L

1 µg% = 10 µg/L

1 γ% = 10 µg/L.

Molarity is the molar concentration, which is expressed in mol/L (or mol/m3, mmol/L, etc.). Conversion factors are listed below:

1 M (molar) = 1 mol/L

1 N (normal) = (1/valency) · mol/L

1 mM (mmolar) = 1 mmol/L

1 Eq/L = (1/valency) · mol/L.

 

In highly diluted solutions, the only difference

 

between the molar and molal concentrations

 

is that the equation “1 L H2O = 1 kg H2O” holds

 

at only one particular temperature (4!C). Bio-

 

logical fluids are not highly diluted solutions.

 

The volume of solute particles often makes up

 

a significant fraction of the overall volume of

 

the solution. One liter of plasma, for example,

 

contains 70 mL of proteins and salts and only

 

0.93 L of water. In this case, there is a 7% differ-

 

ence between molarity and molality. Differ-

 

ences higher than 30% can occur in intracellu-

 

lar fluid. Although molarity is more commonly

 

measured (volumetric measurement), molal-

 

ity plays a more important role in biophysical

 

and biological processes and chemical reac-

 

tions.

376

The activity (a) of a solution is a thermodynamic

measure of its physicochemical efficacy. In physi-

 

 

ology, the activity of ions is measured by ion-sensi-

tive electrodes (e.g., for H+, Na+, K+, Cl -, or Ca2+). The activity and molality of a solution are identical when the total ionic strength ( µ) of the solution is very small, e.g., when the solution is an ideal solution. The ionic strength is dependent on the charge and concentration of all ions in the solution:

µ "0.5 (z12 ! c1 + z22 ! c2 + ... + zi2 ! ci)

[13.1]

where zi is the valency and ci the molal concentration of a given ion “i”, and 1, 2, etc. represent the different types of ions in the solution. Owing to the high ionic strength of biological fluids, the solute particles influence each other. Consequently, the activity (a) of a solution is always significantly lower than its molar concentration (c). Activity is calculated as a = f · c, where f is the activity coefficient.

Example: At an ionic strength of 0.1 (as it is the case for a solution containing 100 mmol NaCl/ kg H2O), f = 0.76 for Na+. The activity important in biophysical processes is therefore roughly 25% lower than the molality of the solution.

In solutions that contain weak electrolytes which do not completely dissociate, the molality and activity of free ions also depend on the degree of electrolytic dissociation.

Fractions (“fractional concentrations”) are relative units:

Mass ratio, i.e., mass fraction relative to total mass

Molar ratio

Volume ratio, i.e. volume fraction relative to total volume. The volume fraction (F) is commonly used in respiratory physiology.

Fractions are expressed in units of g/g, mol/ mol, and L/L respectively, i.e. in “units” of 1, 10–3, 10–6, etc. The unabbreviated unit (e.g., g/g) should be used whenever possible because it identifies the type of fraction in question. The fractions %, ‰, ppm (parts per million), and ppb (parts per billion) are used for all types of fractions.

Conversion: 1% = 0.01 1‰ = 1 · 10–3

1 vol% = 0.01 L/L

1 ppm = 1 · 10–6

1 ppb = 1 · 10–9

Osmolality, Osmotic / Oncotic Pressure

Osmolarity (Osm/L), a unit derived from molarity, is the concentration of all osmotically active particles in a solution, regardless of which compounds or mixtures are involved.

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However, measurements with osmometers as well as the biophysical application of osmotic concentration refer to the number of osmoles per unit volume of solvent as opposed to the total volume of the solution. This and the fact that volume is temperature-dependent are the reasons why osmolality (Osm/kg H2O) is generally more suitable.

Ideal osmolality is derived from the molality of the substances in question. If, for example, 1 mmol (180 mg) of glucose is dissolved in 1 kg

of water

(1 L at 4!C), the molality equals

1 mmol/kg

H2O and the

ideal

osmolality

equals 1 mOsm/kg H2O.

This

relationship

changes when electrolytes that dissociate are used, e.g., NaCl Na+ + Cl. Both of these ions are osmotically active. When a substance that dissociates is dissolved in 1 kg of water, the ideal osmolality equals the molality times the number of dissociation products, e.g., 1 mmol NaCl/kg H2O = 2 mOsm/kg H2O.

Electrolytes weaker than NaCl do not dissociate completely. Therefore, their degree of electrolytic dissociation must be considered.

These rules apply only to ideal solutions, i.e., those that are extremely dilute. As mentioned above, bodily fluids are nonideal (or real) solutions because their real osmolality is lower than the ideal osmolality. The real osmolality is calculated by multiplying the ideal osmolality by the osmotic coefficient (g). The osmotic coefficient is concentration-dependent and amounts to, for example, approximately 0.926 for NaCl with an (ideal) osmolality of 300 mOsm/kg H2O. The real osmolality of this NaCl solution thus amounts to 0.926 · 300 = 278 mOsm/kg H2O.

Solutions with a real osmolality equal to that of plasma (!290 mOsm/kg H2 O) are said to be isosmolal. Those whose osmolality is higher or lower than that of plasma are hyperosmolal or hyposmolal.

Osmolality and Tonicity

Each osmotically active particle in solution (cf. real osmolality) exerts an osmotic pressure (π) as described by van’t Hoff’s equation:

π = R · T · cosm

[13.2]

where R is the universal gas constant (8.314 J · K–1 · Osm–1), T is the absolute temperature in K, and cosm is the real osmolality in Osm · (m3

H2O)–1 = mOsm · (L H2O)–1. If two solutions of different osmolality ( cosm) are separated by a water-permeable selective membrane , cosm will exert an osmotic pressure difference (Δπ) across the membrane in steady state if the membrane is less permeable to the solutes than to water. In this case, the selectivity of the membrane, or its relative impermeability to the solutes, is described by the reflection coefficient (σ), which is assigned a value between 1 (impermeable) and 0 (as permeable as water). The reflection coefficient of a semipermeable membrane is σ = 1. By combining van’t Hoff’s and Staverman’s equations, the osmotic pressure difference (Δπ) can be calculated as follows:

Δπ = σ · R · T · cosm.

[13.3]

Equation 13.3 shows that a solution with the same osmolality as plasma will exert the same osmotic pressure on a membrane in steady state (i.e., that the solution and plasma will be isotonic) only if σ = 1. In other words, the membrane must be strictly semipermeable.

Isotonicity, or equality of osmotic pressure, exists between plasma and the cytosol of red blood cells (and other cells of the body) in steady state. When the red cells are mixed in a urea solution with an osmolality of 290 mOsm/kg H2O, isotonicity does not prevail after urea (σ " 1) starts to diffuse into the red cells. The interior of the red blood cells therefore becomes hypertonic, and water is drawn inside the cell due to osmosis (! p. 24). As a result, the erythrocytes continuously swell until they burst.

An osmotic gradient resulting in the subsequent flow of water therefore occurs in all parts of the body in which dissolved particles pass through water-permeable cell membranes or cell layers. This occurs, for example, when Na+ and Clpass through the epithelium of the small intestine or proximal renal tubule. The extent of this water flow or volume flow Jv (m3 · s–1) is dependent on the hydraulic conductivity k (m · s–1 · Pa–1) of the membrane (i.e., its permeability to water), the area A of passage (m2), and the pressure difference, which, in this case, is equivalent to the osmotic pressure difference Δπ (Pa):

Jv = k · A · Δπ [m3 · s–1].

[13.4]

Dimensions and Units

377

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13 Appendix

378

Since it is normally not possible to separately determine k and A of a biological membrane or cell layer, the product of the two (k · A) is often calculated as the ultrafiltration coefficient Kf

(m3 s–1 Pa–1) (cf. p. 152).

The transport of osmotically active particles causes water flow. Inversely, flowing water drags dissolved particles along with it. This type of solvent drag (! p. 24) is a form of convective transport.

Solvent drag does not occur if the cell wall is impermeable to the substance in question (σ = 1). Instead, the water will be retained on the side where the substance is located. In the case of the aforementioned epithelia, this means that the substances that cannot be reabsorbed from the tubule or intestinal lumen lead to osmotic diuresis (! p. 172) and diarrhea respectively. The latter is the mechanism of action of saline laxatives (! p. 262).

Oncotic Pressure / Colloid Osmotic Pressure

As all other particles dissolved in plasma, macromolecular proteins also exert an osmotic pressure referred to as oncotic pressure or colloid osmotic pressure. Considering its contribution of only 3.5 kPa (25 mm Hg) relative to the total osmotic pressure of the small molecular components of plasma, the oncotic pressure on a strictly semipermeable membrane could be defined as negligible. However, within the body, oncotic pressure is so important because the endothelium that lines the blood vessels allows small molecules to pass relatively easily (σ ! 0). According to equation 13.3, their osmotic pressure difference Δπ at the endothelium is virtually zero. Consequently, only the oncotic pressure difference of proteins is effective, as the endothelium is either partly or completely impermeable to them, depending on the capillary segment in question. Because the protein reflection coefficient σ #0 and the protein content of the plasma (ca. 75 g/L) are higher than that of the interstitium, these two factors counteract filtration, i.e., the blood pressure-driven outflow of plasma water from the endothelial lumen, making the endothelium an effective volume barrier between the plasma space and the interstitium.

If the blood pressure drives water out of the blood into the interstitium (filtration), the

plasma protein concentration and thus the oncotic pressure difference π will rise (! pp. 152, 208). This rise is much higher than equation 13.3 leads one to expect (! A). The difference is attributable to specific biophysical properties of plasma proteins. If there is a pres- sure-dependent efflux or influx of water out of or into the bloodstream, these relatively high changes in oncotic pressure difference automatically exert a counterpressure that limits the flow of water.

pH, pK, Buffers

The pH indicates the hydrogen ion [H+] concentration of a solution. According to Sörensen, the pH is the negative common logarithm of the molal H+ concentration in mol/kg H2O.

Examples:

1 mol/kg H2O = 100 mol/kg H2O = pH 0, 0.1 mol/kg H2O = 10–1 mol/kg H2O = pH 1, and so on up to 10-14 mol/kg H2O = pH 14.

Since glass electrodes are normally used to measure the pH, the H+ activity of the solution is actually being determined. Thus, the following rule applies:

pH = – log (fH · [H+]),

where fH is the activity coefficient of H+. Considering its ionic concentration (see above), the fH of plasma is !0.8.

The logarithmic nature of pH must be considered when observing pH changes. For example, a rise in pH from 7.4 (40 nmol/kg H2O) to pH 7.7 decreases the H+ activity by 20 nmol/ kg H2O, whereas an equivalent decrease (e.g., from pH 7.4 to pH 7.1) increases the H+ activity by 40 nmol/kg H2O.

The pK is fundamentally similar to the pH. It is the negative common logarithm of the dissociation constant of an acid (Ka) or of a base (Kb):

pKa = $log Ka

pKb = $log Kb.

For an acid and its corresponding base, pKa + pKb = 14, so that the value of pKa can be derived from that of pKb and vice versa.

The law of mass actions applies when a weak acid (AH) dissociates:

AH A+ H+

[13.5]

It states that the product of the molal concentration (indicated by square brackets) of the dissociation products divided by the concentration of the nondissociated substance remains constant:

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