Concepts, Phenomena, and Applications
Errata
NOTE: Errata marked with a green checkbox have been corrected in the second printing of the book.
A second printing version is marked by the code 10 9 8 7 6 5 4 3 2 at the bottom of the copyright page of the book.
A first printing version is marked by the code 10 9 8 7 6 5 4 3 2 1.
The content of the book is the same irrespective of the print version.
| Page number | Location | Erratum |
|---|---|---|
| 20 ✅ | Section 1.1 | 140 nanoseconds should become 140 picoseconds. |
| 26 ✅ | Section 1.3.4 | In the last sentence of the first paragraph, the term V ρg should become ρg. |
| 29 ✅ | 1.5 | In the marginnote Gibbs-Duhem should be replaced by Gibbs. |
| 30 ✅ | Section 1.5 | Onsager was awarded the Nobel prize in the 1968, not in 1967. |
| 31 ✅ | Figure 1.9 | In the caption, replace Seebeck coefficient by Seebeck effect. |
| 31 ✅ | Section 1.6.1 | in the second margin note, the term ∂vi∂xj+∂vj∂xi should be ∂vi/∂xj+∂vj/∂xi; moreover, add on after "constraints" earlier in the same sentence. |
| 37 ✅ | Section 1.8 | In this section it is shown that the incompressibility condition (1.48) holds under many circumstances, when the typical length and time scales of the flow are such that their ratio is much smaller than the speed of sound. There can be exceptions though. Consider e.g. flow of a compressible gas through a channel with a thick porous medium. The large pressure difference across the channel will result in a large density gradient along the channel, so mass conservation implies that there will then also be a velocity gradient along the channel. This effect can be important in microfluidics. |
| 36 ✅ | Section 1.19 | Replace Coriolis force by centrifugal force in the caption of Figure 1.11. |
| 48 ✅ | Section 1.13.1 | in the sentence above (1.65) replace ɣsl by ɣsv . |
| 51 ✅ | Section 1.14 | The term p0 in the equation of state is not the same as the one used background pressure used in studying bubble oscillations. It is better to replace p0 in the equation of state by (p0+ 2γ /R0 with p0 the same as the one used in studying bubble oscillations. |
| 51 ✅ | Section 1.1.4 | Just above (1.69), replace (1.66) by (1.67). |
| 55 ✅ | Box 1. | In the third item where the Prandtl number is definited, thermal conductivity needs to be replaced by thermal diffusivity. |
| 56 ✅ | Problem 1.2.b | In the marginnote Gibbs-Duhem should be replaced by Gibbs. |
| 56 ✅ | Problem 1.2 | Replace (1.18) by (1.17) three times: in the heading, in the first and in the last sentence. |
| 56 ✅ | Problem 1.2.b | Change entropy per unit volume by entropy per unit mass. Also, delete the word conservation in the first line. |
| 57 ✅ | Problem 1.3 | the light blue regions should become the darker blue regions. |
| 60 ✅ | Problem 1.9.b | Replace uσ=σ/ρ0 by uσ=√(σ/ρ0). |
| 60 ✅ | Problem 1.9.b | Replace y/(ν/uσ) by y+=y/(ν/uσ). |
| 61 ✅ | Problem 1.10.b | the term gzêz should be gêz. |
| 61 ✅ | Problem 1.10.d | equation (1.86) should be replaced by |
| 62 ✅ | Problem 1.10.e | remove the full stop after equation (1.87). |
| 62 ✅ | Problem 1.10.f | pertubations should be perturbations. |
| 64 ✅ | Problem 1.12 | In the first sentence In this equation should become In this problem. |
| 65 ✅ | Problem 1.13 | In the second row of equation (1.99), z1(r) should be z2(r). |
| 66 ✅ | Problem 1.13 | In equation(1.103) the minus sign on the right hand side should be removed. |
| 508 ✅ | Endnote 32 | 600-800 should be replaced by 1200-1600. |
| Page number | Location | Erratum |
|---|---|---|
| 70 ✅ | Section 2.2 | Before and after equation (2.3), replace strain rate tensor by strain tensor. |
| 70 ✅ | Section 2.2 | In the caption of Figure 2.6, uik should be replaced by uij. |
| 71 ✅ | Section 2.3 | In the lowest marginnote, section I.2.2.b should become section I.2.2.a. |
| 76 ✅ | Section 2.5 | A few lines below equation (2.23), delete As discussed in problem 2.1,. |
| 78 ✅ | Section 2.6.2 | In the second marginnote, replace much less than by much larger than. |
| 88 ✅ | Section 2.8.4 | In the last line of this section problems 2.2-2.4 should become problems 2.3 and 2.4. |
| 88 ✅ | Figure 2.23 | The scale bar in the image should be 4 μm rather than 500 nm as suggested in the figure. Moreover, the snapshots are taken 60 seconds apart, not 4 seconds apart. |
| 96 ✅ | Section 2.10.5 | The combination 3L3Δz/2 appears twice on this page. Both times the factor 3 should be deleted. |
| 98 ✅ | Section 2.10.7.a | Replace μ/K→∞ by μ/K→0, and likewise μ/K→0 by μ/K→∞. |
| 102 ✅ | Section 2.11 | In the upper marginnote on this page, figure 2.37.c should become figure 2.37.b. |
| 107 ✅ | Problem 2.1 | Change the title of problem 2.1. to Derivation of the equations for two simple models for time-dependent response: the Maxwell model and the Klevin-Voigt model. |
| 107 ✅ | Problem 2.3 | In the first line of the problem description, change force Fext ŷ direction direction into force -Fext ŷ. |
| 108 ✅ | Problem 2.3.h | The condition which you should derive reads |
| 109 ✅ | Problem 2.5.a | The reference should be to equation (2.56) instead of to equation (2.57). |
| 110 ✅ | Problem 2.7 | ..rest length A should be ..rest length a. |
| 113 ✅ | Problem 2.7.h | In equation (2.101) the term in the nummerator on the right hand side should read ∂2Dim. |
| 116 ✅ | Problem 2.8.a | After equation (2.122), replace strain rate tensor by strain tensor. |
| 116 ✅ | Problem 2.7.p | Replace k/2 by k/(2√3). |
| 117 ✅ | Problem 2.8.c | After equation (2.125), replace strain rate tensor by strain tensor. |
| 117 ✅ | Problem 2.8.e | In the caption of figure 2.41, replace π/6 by π/3. |
| 118 ✅ | Problem 2.8.g | Add the marginnote Note that in the field of liquid crystals, it is common to write the defect strength s in units of 1/2. We follow that different convenction in Chapter 6. |
| 118 ✅ | Problem 2.8.g | Replace the sentence between brackets after (2.134) into (i.e., s=2π/6> corresponds to five nearest neighbors, s=−2π/6 corresponds to seven). Also, take out the factor 2π/6 from equation (2.134) and the factor π/3 from equation (2.135. |
| 118 ✅ | Problem 2.8.g | Change collection of dislocations into collection of disclinations. |
| 509 ✅ | Endnote 4 | is still 11 should be replaced by is still 13. |
| 509 ✅ | Endnote 19 | Fel,x = Fext should be replaced by Fel,x = -Fext. |
| 511 ✅ | Endnote 45 | The reference to the paper Miskin and Jaeger, 2013 should be replace a reference to Goodricht et al., 2015. |
| Page number | Location | Erratum |
|---|---|---|
| 127 ✅ | Section 3.25 | In equation (2.34) take out the term Γ-1 in the left equation. Furthermore, add the lower integration boudary -∞ to the integral in the right equation. In (3.25) replace 2γΓ by γ/Γ. |
| 128 ✅ | Section 3.3.5. | In equation (3.38), add a factor D to the right hand side. |
| 133 ✅ | Section 3.3.6 | Replace the last line ("Quite.... term.") of section 3.3.6 by Nevertheless, as the prefactor itself does not depend on the temparature (as D is proportional to T), the temperature dependence of the transition rate comes completely from the exponential term. |
| 134 ✅ | Section 3.4 | In the right hand side of equation (3.43), kBT should be replace by 2kBT in the exponent of the expression for Wnn'. |
| 147 ✅ | Problem 3.1.a | Change as follows. The into through steps a and b below. Start by checking that the |
| 151 ✅ | Problem 3.6.d | The derivatives d/dx should be replaced by partial deriviatives ∂/∂x. |
| 153 ✅ | Problem 3.8 | kT should become kBT in equations (3.88) and (3.89). |
| 160 ✅ | Problem 3.11 | In the marginnote, section 3.7.2 should become section 3.6.1. |
| 511 ✅ | Endnote 3 | Replace law of large numbers by central limit theorem. |
| Page number | Location | Erratum |
|---|---|---|
| 191 ✅ | Problem 4.3.e | introducting shoud be introducing. |
| 199 ✅ | Problem 4.11 | ... boiling of water, melting a two-dimensional crystal, and the onset of ferromagnetism. shoud be ... the critical points of liquids, critical liquid demixing, and the onset of ferromagnetism. |
| 201 ✅ | Equation (4.63) | delete the comma after the first row. |
| Page number | Location | Erratum |
|---|---|---|
| 204 ✅ | Figure 5.2 | In the caption François Tournillac should be François Tournilhac. |
| 249 ✅ | Equation (5.90) | s1 – s2 should become |s1 - s2|. |
| Page number | Location | Erratum |
|---|---|---|
| 278 ✅ | Section 6.6.1.a | Add the marginnote Note that we here follow the liquid crystal literature by defining the defect strength s in units of 1/2, whereas in elastic media units of π/3 are used (see problem 2.18 and chapter 7). |
| 296 ✅ | Problem 6.1.e | a in equation (6.58) should be replaced by D. |
| 297 ✅ | Problem 6.2.d | note that the expression you are asked to derive is actually for the entropy per unit volume. |
| 303 ✅ | Problem 6.8.b | The definition |
| Page number | Location | Erratum |
|---|---|---|
| 335 ✅ | Problem 7.5.c | h=bχ should be h → bχ h. |
| 337 ✅ | Problem 7.8 | see section .a should be see section 7.4.1.a. |
| 343 ✅ | Problem 7.11 | After equation (2.122), replace strain rate tensor by strain tensor. |
| Page number | Location | Erratum |
|---|---|---|
| 367 ✅ | Figure 8.14 | In the figure, in the right panel zero wavelength should be zero wavenumber. |
| 367 ✅ | fourth row of second paragraph | "...it is a zero wavelength..." should be "...it is a zero wavenumber...". |
| 369 ✅ | lowest margin note | for this case g<0 should be for the case g<0 |
| 397 ✅ | Problem 8.3 | step j should be labeled f. |
| 398 ✅ | Problem 8.4 | Note that steps d, e and f can best be solved together. |
| 398 ✅ | Problem 8.4.e | In the last sentence of the paragraph, zero wavelength should be zero wavenumber. |
| 398 ✅ | Problem 8.5 | in the upper row of equation (8.85): the term (b+1) should be replaced by (b+1)u1. |
| 401 ✅ | Problem 8.8.e | equation (8.8) should be equation (8.9). |
| Page number | Location | Erratum |
|---|---|---|
| 411 ✅ | 5 lines below (9.12) | polarizatation should become polarization. |
| 414 ✅ | 1st sentence of 2nd paragraph | gate should become gait. |
| 419 ✅ | Figure 9.12 | The scale bar in the top figure denotes 100 micron rather than 15 micron. |
| 444 ✅ | Problem 9.2.j | All the terms involving J in equation (9.102) should be replaced by 2πJ. In addition, ∂z should be substituted with ∂z̄ and vice versa in all terms. |
| 445 | Problem 9.3 | Note that (9.107) unfortunately has the opposite sign of α from that used in the main text of chapter 9, and in the previous problem 9.2.k. We keep the different sign in the solution worked out in the solution manual, and, for consistency between the versions, also in problem 9.3 in second printing of the book. |
| 447 ✅ | Problem 9.3.h | The expression (9.120) for c2(θ) is wrong. It should be . |
| 449 ✅ | Problem 9.4.c | …into (9.125) should become …into (9.126). |
| 451 ✅ | Problem 9.5.e | and linearize (9.137) should be and linearize (9.138). |
| 453 ✅ | Problem 9.7.e | The full stops before equations (9.152) and (9.153) should be removed. In equation (9.153) both logarithms should be natural logarithms ln, and divided by the length scale L that first appears in equation (9.151). |
| 453 ✅ | Problem 9.7.e | In equation (9.153) a term 1/n should be included in the summand (i.e., insert a term 1/n between the summation sign and the term in brackets). In addition log should be replaced by the natural logarithm ln twice. |
| 458 ✅ | Problem 9.12.d | Find the intersections of κ3 some constant with f(θ). should be Find the intersections of κ3 = const. and κ3= f(θ). |
| 459 ✅ | Problem 9.12.i | This problem duplicates 9.12.e and can be skipped. NB: the problem has been deleted in the second printing. |
| Page number | Location | Erratum |
|---|---|---|
| 578 ✅ | figure 4.14.a | E.R Week should be E. R. Weeks. |
| 578 ✅ | figure 5.2 | F. Tournillac should be F. Tournilhac. |
| 579 ✅ | figure 9.13 | N. Fahkri should be N. Fakhri. |
| 579 ✅ | figure 9.23 | H. Tullier should be H. Turlier. |