Descriptive Physical
Oceanography: An Introduction (Sixth Edition)
Talley,
Pickard, Emery and Swift
Elsevier, 2011
Corrections
As
of September 26, 2015
Chapter 1:
Figure 1.2: ÒTsunamisÓ should be placed on the
graph with frequency range 1min-20 hours, rather than the higher frequency
range.
Chapter 3:
Section 3.4 (p.
36): ÒAdvances in electrical circuits and sensor systems permitted accurate
compensation for temperature, making conductivity-based salinity measurements
feasible (see supplemental materials in Chapter S16,
Section S16.4.3 on the textbook Web site).Ó
Section 3.5.5
(pp. 43-44) To standardize definitions of thermal expansion and haline contraction:
ÒAs
described above, the equation of state (3.6) is somewhat nonlinear in
temperature, salinity and pressure.
That is, the equation of state (EOS 80) includes products of salinity,
temperature and pressure.
Sometimes, for practical purposes, in theoretical and simple numerical models
the equation of state is approximated as linear and its pressure dependence is
ignored:
r Å r0 - ar (T-T0) + br (S-S0); a = -(1/r) ¦r/¦T and b = (1/r) ¦r/¦S |
(3.9) |
where r0, T0 and S0
are arbitrary constant values of r, T and S; they are usually
chosen as the mean values for the region being modeled. Here a is the thermal expansion coefficient, which expresses the change in
density for a given change in temperature (and should not be confused with
specific volume, defined with the same symbol in section 3.5.3) and b is the haline contraction coefficient, also called the saline contraction coefficient, which is the change in density for
a given change in salinity. The
terms a
and b
are nonlinear functions of salinity, temperature and pressure; their mean
values are chosen for linear models.
Full tables of values are given in UNESCO (1987). The value of a (at
the sea surface and at a salinity of 35 g kg-1) ranges from 53 x 10-6
K-1 at a temperature of 0¡C to 257 x 10-6 K-1
at a temperature of 20¡C.
The value of b (at the sea surface and at a salinity of 35 g kg-1) ranges from
785 x 10-6 kg g-1 (at a temperature of 0¡C) to 744 x 10-6
kg g-1 (at a temperature of 20¡C).Ó
Figure 3.7 caption edit. ÒFor
a station in the Pacific Ocean ÉÓ
(delete ÒPapaÓ)
Chapter 4:
Figure 4.17a: edited to
remove title and page number from original scan.
ÒFIGURE 4.24 (a)
Chlorofluorocarbon content (CFC-11; pmol/kg) and (b) D14C (/mille)
in the Pacific Ocean at150¡W. Dark cyan (gray) areas in (a) indicate undetectable CFC-11. From
the WOCE Pacific Ocean Atlas. Source: From Talley (2007).Ó
Chapter 5:
ÒFIGURE
5.17 Sverdrup transport (Sv), where negative is
clockwise and positive is counterclockwise circulation. Wind stress data are
from the NCEP reanalysis 1968-1996. (Kalnay
et al., 1996). The wind stress and wind stress curl used in this
Sverdrup transport calculation are shown in the online supplement, Figure
S5.10.Ó
Section 5.4.3 (p. 124): ÒDirect measurements of the energy arriving at the sea surface are
made with a pyranometer (see Section S16.8 located on the textbook Web site), but it is not
practical to do this over large areas, or for prediction.Ó
Section 5.4.4.1 (p. 128): ÒIt is difficult to
directly measure Qb over large areas, although it can be measured
locally with a radiometer (see the description in Chapter
S16, Section S16.8 located on the textbook Web site).Ó
Section 5.4 clarification:
The net air-sea heat flux Q is given by Eqs. 5.8 and 5.9. The signs of the individual terms in Eqs.
5.10 through 5.17 are not provided in a manner that is consistent with Eqs. 5.8 and 5.9. The shortwave
radiation (5.10) is positive for heat gain by the ocean. The longwave radiation (5.11) is
positive for heat loss from the ocean.
The latent heat loss (5.13) is positive for heat loss from the ocean. The sensible heat loss (5.17) is
positive for heat loss from the ocean.
The maps of air-sea heat flux (Figs. 5.11, 5.12, and supplementary
figures), positive heat flux means the ocean is gaining heat. For these definitions and for the maps
then, Equation (5.8) should be written as:
QT = Qs - Qb - Qh - Qe +
Qv (5.8)
and similarly for Equation (5.9):
Qs - Qb - Qh - Qe = Qsfc (5.9)
Table
5.2: Header should read ÒSome Values for the Sensible Heat Transfer Coefficient
at 10 m, 103Ch, as a Function of (Ts – Ta)
and Wind Speed uÓ
Chapter 7
Corrected
caption (in print chapter, and also color plates and online powerpoint):
ÒFIGURE 7.8 Ekman response.
Average wind vectors (red/black) and average
ageostrophic current at 15 m depth (blue/gray).
The current is calculated from 7 years of surface drifters drogued at 15 m,
with the geostrophic current based on average density data from Levitus et al.
(1994a) removed. (No arrows were plotted within 5 degrees of the equator
because the Coriolis force is small there.) This figure can also be found in
the color insert. ©American Meteorological Society.
Reprinted with permission. Source: From
Ralph and Niiler (1999).Ó
Equation (7.27a) in Section 7.6.2 is missing
the ' for r in the integrand:
h' = - (1/ro ) ˜ r' dz (7.27a)
Section 7.8.3 references Munk (1950), which is
missing in the DPO reference list.
Munk, Walter H., (1950). On the wind-driven ocean. J.
Meteor., 7, 80–93.
Chapter S7 (supplement)
ÒFIGURE S7.30 (a) Rossby deformation radius (km) for the first baroclinic mode (Chelton et al., 1998). (b) Shortest period (in days) for the first baroclinic mode, based on the deformation radius in (a). Note that the annual cycle, at 365 days, occurs around latitudes 40¡ to 45¡; poleward of this, all such waves are slower (Wunsch, 2010).Ó
Wunsch,
Carl, 2010: Toward a Midlatitude Ocean
Frequency–Wavenumber Spectral Density and Trend
Determination. J. Phys. Oceanogr., 40, 2264–2281.
Chapter 8
First paragraph should read: ÒThis chapter continues the dynamical discussion of Chapter 7,
starting with an overview of the properties of waves (Section 8.2), and moving to
surface and internal gravity waves and tides (Sections 8.3 to 8.6).Ó The second sentence should be deleted,
as there is no expanded version.
Section 8.6.2, pp. 240-241: ÒThe spring and
neap tides are illustrated in Figure 8.13 using a two-month record at La Jolla.Ó
Chapter 9
Figure 9.1b: arrow
indicating circulation direction around Zapiola Rise is incorrect,
should be counterclockwise (anticyclonic).
Chapter 10
Corrected caption
ÒFIGURE
10.29 Potential T-S curves for selected stations (inset map).
Acronyms: NPCW, North Pacific Central Water; SPCW, South Pacific Central Water;
NPSTUW, North Pacific Subtropical Under- water; SPSTUW, South Pacific
Subtropical Underwater; NPSTMW, North Pacific Subtropical Mode Water; SPSTMW,
South Pacific Subtropical Mode Water; NPIW, North Pacific Intermediate Water;
AAIW, Antarctic Intermediate Water; DtW, Dichothermal Water; MtW, Mesothermal
Water; CCS, California Current System waters; and PCCS, Peru-Chile Current
System Waters. This figure can
also be found in the color insert.Ó
[Delete second to last sentence in original caption.]
Chapter 11
Figure
11.1b. The current labeled
ÒNorthwest Monsoon C. (NEC)Ó should read ÒNortheast Monsoon
C. (NEC)Ó
Click here for link to corrected figure.
Chapter S12:
Figure S12.4. Figure panel included extra text.
Click here for link to corrected figure.
Chapter 13:
p. 449
(section 13.3.2): SPZ and SZ are reversed. See Table 13.1 and Figure 13.4 for
correct locations. Correct text
is: ÒThe SZ lies
between the SACCF and SB. Within the SZ, the low
oxygen UCDW upwells to the surface and is converted to very cold ASW.
The SPZ
lies between the SB and the Antarctic Shelf Front.Ó
Chapter 14:
Figure 14.2.
Panel (a) and (b) captions are reversed. Correct caption:
ÒFIGURE 14.2 (a) Surface
velocity streamlines, including both geostrophic and Ekman components; color is
the mean speed in cm/sec, and (b) surface dynamic topography (dyn cm), with 10
cm contour intervals. This figure can also be found in the color insert. Source: From Maximenko
et al. (2009).Ó
Equation 14.1a, b: correction so that sign of W
is positive upwards.
MTi = VNi - VSi + Wi - Wi-1
= 0
Wi = - VNi + VSi + Wi-1 (14.1a, b, c)
wi = Wi/Ai
Chapter S14:
Figure S14.8. Incorrect
figure from Davis (2005).
Click here for link to corrected figure.
Chapter S15:
Figure S15.9. Panel (a) and (b) captions are reversed. Correct caption:
ÒFIGURE S15.9. Indian Ocean
Dipole mode. (a) IOD index (blue: difference in SST anomaly between the
western and eastern tropical Indian Ocean), plotted with the anomaly of zonal
equatorial wind (red) and the Nino3 index from the Pacific (black line). (b) Anomalies
of SST (shading) and wind velocity (arrows) during a composite positive IOD
event. These are accompanied by higher precipitation in the warm SST region and
lower precipitation in the cool SST region. Source: From Saji et al.,
(1999).Ó
Typos:
Chapter S15, p.
25, para. 2 line 2, extra space before comma
References (missing)
Munk,
Walter H., (1950). On the wind-driven
ocean. J. Meteor., 7, 80–93.