Thread about Jackson's Classical Electrodynamics 3rd edition

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The discussion revolves around clarifying derivations in Jackson's "Classical Electrodynamics" 3rd edition, specifically regarding Taylor expansions and the behavior of integrals involving charge distributions. A key point is understanding why certain linear terms vanish in the Taylor expansion, attributed to symmetry in the integrals over spherical domains. Participants also discuss the implications of these calculations on the behavior of electrostatic potentials and charge distributions, referencing specific problems from the textbook. Additionally, there are inquiries about the correctness of solutions provided in external resources, indicating a collaborative effort to resolve complex derivations. The thread aims to enhance comprehension of these advanced topics for students and professionals alike.
  • #31
I am reading now the solution of problem 3.19 from Jackson (if you know of another more complete solution let me know);

here:
http://homerreid.dyndns.org/physics/jackson/jack3c.pdf

And it seems he's stuck at calculating the integral ##\int_0^\infty \frac{\sinh(kz_0)}{\sinh(kL)}kdk##, can you help both of us?

Thanks in advance!
Cheers!
 
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  • #32
I read someone's remark on solving Jackson's problems:
"Getting any single Jackson problem completely correct could be a life’s work!"

LOL! wish I had the time to solve completely correctly the 350 problems in the third edition, but I have exams... :-D
 
  • #33
Mathematica gives as a result (of course only valid for ##L>z_0##)
$$\frac{1}{4L^2} \left [\psi'\left (\frac{L-z_0}{2L} \right )-\psi' \left(\frac{L+z_0}{2L} \right ) \right ],$$
where
$$\psi(z)=\frac{\Gamma'(z)}{\Gamma(z)}$$
is the socalled "digamma" function.
 
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  • #34
vanhees71 said:
Mathematica gives as a result (of course only valid for ##L>z_0##)
$$\frac{1}{4L^2} \left [\psi'\left (\frac{L-z_0}{2L} \right )-\psi' \left(\frac{L+z_0}{2L} \right ) \right ],$$
where
$$\psi(z)=\frac{\Gamma'(z)}{\Gamma(z)}$$
is the socalled "digamma" function.
Does this expression simplifies to the expression in problem 3.19 in Jackson's? i.e with the ##\sec^2##?
 
  • #36
I have a question regarding problem 5.5 from Jackson's third edition.

Do I actually need to post it (I mean I assume that you have a legal or illegal copy of the book).

I've found a solution to problem 5.5 from here:
http://pages.uoregon.edu/gbarello/Resources/Papers/Homework/Electrodynamics/HW4.pdf
on page 8 the solution to assignment 5.5b, the last solution has the wrong coefficients, so I wonder where did he go wrong there?

Thanks, jesus and out... :-)
 
  • #37
Does someone know if some of the problems in Jackson's third edition can be found in reference books?

There are some problems about superconducting material which I thought may be found in Tinkham's reference.
 
  • #43
vanhees71 said:
Admittedly the calculation is a bit confusing, because of the shorthand notation used by Jackson. Calculated is the volume integral

For ##n \geq 2## I cannot verify generally Jackson's result, but all you need is to show that the integral is 0 for ##a \rightarrow 0##. Now introduce again spherical coordinates, and you see that all these integrals are proportional to
$$3 a^2 \int_0^R \mathrm{d} r \frac{r^{n+2}}{(r^2+a^2)^{5/2}}=3a^2 I_n.$$
[corrected in view of the hint in #7]
For ##n=2## we get
$$I_2=\int_0^R \mathrm{d} r \frac{r^{4}}{(r^2+a^2)^{5/2}}=\mathrm{arsinh} \left ( \frac{R}{a} \right )-\frac{4R^3+3ra^3}{4(R^2+a^2)^{3/2}}.$$
Obviously one has
$$\lim_{a \rightarrow 0} a^2 I_2=0.$$
I'm not very good in curvilinear coordinates, let me try to expand it in cartesian coordinates instead. I'm not sure whether the reasoning is correct though (note that odd components of ##\mathbf{h} = |\mathbf{x^{'}} - \mathbf{x}|## cancel)...
\begin{align*}
\rho(\mathbf{x}^{'}) & =\rho(\mathbf{x}) + \frac{1}{1!}\frac{\partial \rho}{\partial \mathbf{h}} +\frac{1}{2!}\frac{\partial^2 \rho}{\partial \mathbf{h}^2} + \cdots\\
&=\rho(\mathbf{x}) + (\mathbf{x^{'}} - \mathbf{x})\cdot\nabla \rho + (\sum_{i} (x^{'}_{i} - x_{i} \frac{\partial}{\partial e_{i}}))(\sum_{i} (x^{'}_{i} - x_{i} \frac{\partial}{\partial e_{i}}))\rho + \cdots\\
&=\rho(\mathbf{x}) + \frac{1}{2} ( (x^{'} -x)^2 \frac{\partial^2 \rho}{\partial x^2} + (y^{'} -y)^2 \frac{\partial^2 \rho}{\partial y ^2}+ (z^{'} - z)^2 \frac{\partial^2 \rho}{\partial z^2})+ \cdots\\
&=\rho(\mathbf{x}) + \frac{|\mathbf{x^{'}} - \mathbf{x}|^2}{6} ( \frac{\partial^2 \rho}{\partial x^2} + \frac{\partial^2 \rho}{\partial y ^2} + \frac{\partial^2 \rho}{\partial z^2})+ \cdots\\
&=\rho(\mathbf{x}) + \frac{r^2}{6}\nabla^2 \rho + \mathcal{O}(r^3)
\end{align*}
Since ##\rho## does not vary much in the volume of interest we may assume the function is spherically symmetric, we see that $$ (x^{'} -x)^2 \frac{\partial^2 \rho}{\partial x^2} \approx (y^{'} -y)^2 \frac{\partial^2 \rho}{\partial x^2}$$

and $$ 3 (x^{'} -x)^2 \frac{\partial^2 \rho}{\partial x^2} \approx |\mathbf{x^{'}} - \mathbf{x}|^2 \frac{\partial^2 \rho}{\partial x^2}$$

Right?...
 
  • #44
By the way, judging by how seasoned the advice Jackson gives, how comprehensive the treatment is and the copious amounts of references given, I wonder, did Jackson actually read through all the books he cite? (or at least read a few chapter)
 

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