- In Example 2.2 on p.27, on the right of the two equations for computing
the air drag force, the terms (B2/m) should read B2.
Thus the equations should have been:
Fdrag,x = - B2 v vx,i,
Fdrag,y = - B2 v vy,i
We appreciate the help by Jeff de Jong for finding this and a few other errors.
- On p.22, as noted in footnote 5, the definition of the drag coefficient
C was changed by a factor of 2 from the first edition of this book
(cf. Eq.(2.9)). This actually corrected an implicit error in that edition
in presenting the measured values of C in Figure 2.6 as well as to
conform better to the standard definition. On the other hand, in section 2.5
on Golf, we continued to use the old definition of C in Eq.(2.34).
Thus the discussion of numerical values of C in section 2.5 corresponds
to half of the values of the drag coefficient in the analogous discussion
on the baseball in previous sections. This invites confusion and we regret
that we had not unified the definition of C in all sections.
Thank you for Jeff de Jong for raising this issue.
In addition, Charles Maguire pointed out that the caption of Figure 2.2 on
p.23 quotes an incorrect value of the drag coefficient; while it states
C=0.5 was used, it should have been C=1 instead
according to the new definition in this edition of the book.
- On p.48, just preceeding Eq.(3.1), we state that "The parallel forces
add to zero, since we assume that the string doesn't stretch or break".
This is incorrect except at the highest points of the pendulum where
its velocity is zero since the net parallel force must provide the needed
centripetal acceleration to keep the pendulum in motion along a circular arc.
We thank John Goff and William DeBuvitz for alerting us to this error.
- On p.49, 4th line from the top, "where l is the length of
the string" should be changed to "where l is the length of the string
and
is measured
in radians. (Pointed out by William DeBuvitz.)
- In Example 3.3 on p.58, there are 2 typos in the signs for the
time evolution equation for
. The minus sign in front of
the bracket should be a plus and there needs to be a minus within the brackets
in front of the term (g/l) sin
i.
Thus, the corrected equation should read:
i+1 =
i
+
[- (g/l) sin
i
- q
i
+ FD sin (
D ti) ]
t
We are grateful to Denis Donnelly for pointing this out.
- On p.98, the last row of Table 4.1 gives an incorrect value for
the mass of Pluto. It should read
1.3
1022 kg.
We appreciate the help by Charles Maguire on this point.
- On p.125, in the expression for the moment of inertia I just
after Eq.(4.23), |r1| and |r2|
are meant to be the distances from the center of mass of the two particles
to each of the particles (and not from Saturn at the origin). This notation
was at best unclear as John Goff pointed out. This part should have read
where I = m1d12 +
m2d22 is the moment of inertia and
the distances d1 and d2 are measured
from the center of mass of the two particles to each particle.
- On p.131, line 6 from top and paragraph 2, line 5 and
again on p.138, paragraph 3, line 2,
we refer to Fig. 12.47 where we should have referred to
Fig. 5.1 instead.
We have no idea why this happened and since there is a totally unrelated
Fig. 12.47 later on, it is a confusing error.
We thank Gus Hart again for spotting this problem.
On line 3 and the last line on p.193, references to Table 7.3 appear.
The references should be Table 7.1 on the same page instead.
- In Eq.(7.20) on p.196, there should be a factor of D on the right-hand
side of the equation. Thank you, Geron Bindseil for bringing this to our
attention.
- On p.220, The text that appear in the 2nd tertiary bullet (dark dot)
of Example 7.4 should have been enclosed within a box.
- On p.221, just above Example 7.5, the reference to "the box in Example
7.8" should have been to "the box in Example 7.4". This is the text that
should have appeared within a box but didn't (see above). Thanks to
Bernhard Gubanka for noticing this error.
- On p.225, just after Example 7.6, the reference to the Depth-first
algorithm described in "Example 7.3" should have been to "Example 7.2".
- On p.229, at the beginning of the last paragraph, "Another consequence
effect of ..." should read "Another consequence of ..."
- On p.265, just after Eq.(8.32), the equation defining t that
appears in Eq.(8.32) should have read
t
1 - zJ/kBT
(T-Tc)/Tc. In other words, the equality should
have been an approximate equality since we
have replaced T in the denominator by Tc where
T is near Tc. This has been pointed out by
John Goff. (Please note that we have defined t here as the
coefficient of the term linear in m in Eq.(8.32) that came from
Eq.(8.31), and thus did not define it as (T-Tc)/Tc
as might be more commonly done. Of course, the two expressions are nearly
equal near the critical point anyway.)
- On p.274, in the 3rd line from bottom, the reduced unit of time for Ar
is given as 1.8
10-12 sec, but it should have been
2.2
10-12 sec instead. This is one of the many errors pointed
out by Bernhard Gubanka.
- On p.280, in Eq.(9.9), v2/kBT should be replaced by
v/kBT. The
prefactor of the exponential in d-dimensions generally is proportional
to vd-1 (kBT)-d/2. Also, Eq.(9.10) is the
correct distribution of the x-component of the velocity in any
dimensions. There, you simply disregard the values of the other component(s)
and just look at how vx is distributed between negative infinity
and positive infinity; then you get (9.10). We thank Charles Maguire for
making us aware of the issues with these equations.
- In Eq.(9.17) on p.296, the two factors of
(
t)2 in the denominators should both
be in the respective numerator. We are grateful to Gus Hart for
pointing out this error. Thus the corrected equation should read:
xi(n+1) = 2 xi(n) - xi(n-1)
+ (
t)2
[ xi+1(n) + xi-1(n) - 2 xi(n) ]
+
(
t)2
( [ xi+1(n) - xi(n) ]3
+ [xi-1(n) - xi(n) ]3 )
- There is a typo in the second bullet of Example 10.1 on p.311.
The initial values of
should be non-zero. That is,
we should have
0 =
-1 =
1, e.g., and not 0.
We are grateful to Katie Sweet for pointing out this error.
- On p.317, in Fig. 10.8, we stated that the solutions from left and right
match fairly well for E=-1.969. While they do match better for this energy
than for E=-1.6, the error is still substantial. Much better match is obtained
for about E=-1.890, and thus the latter vaule would be an acceptable solution,
but not E=-1.969. Again, thank you, Bernhard Gubanka.
- On p.327, third line from the top, the reference to Eq.(10.17) should
have been to Eq.(10.18) as φ is a proposed solution for
the Hamiltonian (10.17) and not of it. Rather, it is a poposed
solution of (10.18). Thanks to Olle Windelius for pointing this out.
- There is a typo in Eq.(10.41) on p.335 pointed out by several readers
(including Trevor Byrne).
The last term on the right should have a plus sign in front, not the minus.
The corrected equation should read:
R(x,t+
t)
R(x,t) -
[
t/2(
x)2]
[ I(x+
x,t+
t/2)
- 2 I(x,t+
t/2)
+ I(x-
x,t+
t/2) ]
+
(
t) V(x) I(x,t+
t/2)
- On p.339, the calculation for the Fig. 10.17 was performed using
the Crank-Nicholson method (rather than the leap-frog method) and this
should have been mentioned for clarity as the stability conditions are
different for the two methods.
- On p.345, there is a typo in Eq.(10.56) pointed out by Elie Kawerk.
On the last line of the equation, in the numerator, the term
R(x,y+
x,t) should have been
R(x,y+
y,t). Also note, as stated at the top
of p.346, we have already set
x=
y on that line
to get the denominator to be
(
x)2.
- On p.384, the second line of Eq.(11.31) should read:
p(i,n+1) = p(i,n) - ...
that is, the second index of p(,) on the right had side should be n
instead of n-1.
- On p.440, in the second line of Eq.(12.23) the exponent -V/20
should read -V/80. That is, that line should be
n = 0.125 e-V/80 .
- This is not an error per se, but in Appendix A.3, we discuss
the Verlet method and its local error of
O[(
t)4]. Gus Hart has made a rather
interesting observation that the application of the Verlet method to the
exactly solvable problem of the simple harmonic oscillator produces a
cumulative error of O[(
t)2]
rahter than the naively expected one of
O[(
t)3]. This turns out to be true
also for the radioactive decay problem. There are some arguments we could
make for this unexpected behavior as a general result (under certain
assumptions) due to the faster accumulation of the local errors
by virtue of the way Verlet time evolution works (A.19). So the analysis
has an interesting twist that neither author was aware of. This point
will be further investigated and may possibly be incorporated in a future
edition.
- In Appendix B.2 on p.472, there are some typos. First, on the 5th line
of B.2, "x1 < x2 < x3" should read
"xa < xb < xc". Second, in Example B.1,
in the 3rd bullet, "g(x0)
g(x1)"
should read "g(x0)
g(x1)".
This error was pointed out by Jeff de Jong.
- In Appendix C.1 on p.480, lines 1 and 2, "sines of cosines" should
read "sines and cosines".
- In Appendix C.4 on p.488, line 2, the refernce to Fig. A2.4 should
be one to Fig. C.4 instead. This and the previous
errors were pointed out by Gus Hart (as were many others).
- On p.490, there are two embarassing errors. In Eq.(C.13), the integration
is over t, not
. So d
should be replaced by dt. In Eq.(C.14),
the integral should be double, over both t and
.
So there should have been an inner (or outer) integral
-
... dt
on the righthand side. These errors were discovered by Bernhard Gubanka.
- About midway down on p.498, the equation that footnote 6 should be
referencing is (D.18) but it appears as (??). Thanks, Len Finegold for
pointing this out.
- On p.502, in Eq.(E.9), a factor of
x is missing
on both terms on the right as pointed out by Dr. Anselmo.
- On p.518, in Eq.(F.4), a minus sign is missing in the exponent.
- On p.527, in the 5th line from top, "was also be" should read
"can also be".
- Equations (H.4) and (H.5) in Appendix H on p.528 have misprints.
The last terms on the left-hand side of these equations should be
a1NxN and
a2NxN, respectively.
The "xN" in these terms were erroneously shown as "x1"
and "x2", respectively, in the published version.
- On p.534, just after Eq.(H.27), A x = f
should be replaced by A x = b. On the same page,
just after Eq.(H.30), E(n) should be replaced by
En (i.e., E raised to the n-th power).