regarding the last step in the proof of Lemma 5.8, namely the convergence un→u, isn't this just the usual argument that Bnfn→Bf for a sequence (Bn) of operators between to Banach spaces that converges strongly to B and a sequence fn that converges to f in the norm of the first Banach space?
Best wishes, Hendrik
Christian Seifert, 2023/01/22 20:08
Dear Hendrik,
Many thanks. Yes, this is indeed the abstract argument.
Best,
Christian
Hendrik Vogt, 2023/01/23 16:17
Dear Chistian,
thanks for the feedback!
Best wishes, Hendrik
Ragon Ebker, 2022/12/28 19:10
Hello,
In Lemma 5.9 we talk about a w0 but it is nowhere defined, should that be a w?
Greetings
Ragon
Jonathan Mui, 2022/12/31 03:03
Hi Ragon,
It seems to me that w0 is the initial condition for the supersolution w, i.e. w0=w(0).
Cheers,
Jonathan
Christian Seifert, 2023/01/02 10:52
Dear Ragon and Jonathan,
Yes, w0 is the initial condition of w.
Best,
Christian
Anna Muranova, 2022/12/26 19:36, 2022/12/26 19:36
Dear authors,
in the proof of the Theorem 5.15 (i′)⇒(ii) shouldnt the contraction C[0,1α] used instead of C[0,α]?
Best,
Anna
Christian Seifert, 2023/01/02 10:49
Dear Anna,
Many thanks; you are absolutely right.
Best,
Christian
Sahiba Arora, 2022/12/23 14:25
Dear all,
I have a small question concerning Theorem 5.15. In condition (ii), is “for every” equivalent to “for some” α>0?
Regards,
Sahiba
Sascha Trostorff, 2022/12/12 15:31
Dear ISEM-Team,
I have a question concerning Exercise 7.1: Shouldn't we assume that c=0? Otherwise the statement seems to be wrong (just consider X={x} to be a singleton and c(x)=1).
Best regards
Sascha
Christian Seifert, 2022/12/13 12:54
Dear Sascha,
Many thanks. Indeed, we should assume c=0 there.
Best,
Christian
Robert Haller, 2022/12/07 11:00, 2022/12/07 11:00
Dear virtual lecturers,
in the discussions in the Darmstadt team we found several times that what we are truly missing is some sort of reference example of a graph, that helps to see the effects described in the text. In particular the behavior of solutions to the heat equation should be something that has an obvious physical intuition and it would be nice to see this in some concrete example.
I try to explain what I mean: I always try to compare the results with the situation in spatial domains that I know better and there for instance the domain monotonicity described in this lecture is something completely intuitive and it becomes also clear there why it only works for Dirichlet boundary conditions and not for Neumann conditions. I am still lacking an intuition what the “boundary conditions” mean here, as there is no apparent boundary in the graphs and I would hope to see the difference of these boundary conditions in a concrete example.
Is something like this possible and will there be some examples in future lectures?
Finally one remark about the text of lecture 7: In the proof of Lemma 5.3 (b) (line 22 ff of page 85) you want to show that x↦e−tx belongs to A for all t≥0. As you later prove that A equals C0([0,∞)) that cannot be true for t=0, as then this function is constantly one and thus does not belong to this space. In fact you probably mean that the assertion of the Lemma is obvious for t=0 and the argument given gives the assertion for all t>0.
Best regards,
Robert
Christian Seifert, 2022/12/13 12:52
Dear Robert,
Many thanks for the comment and remark.
Indeed, we will provide some class of examples in the last lecture.
Best,
Christian
Ragon Ebker, 2022/12/30 05:04
Hello Robert,
It helped me a lot to work through the examples and applications which are given in Chapter 0 in the book. Especially in Chapter 0.4 and 0.5. Also there are special Example exercises for classic graphs (star graphs, line graphs etc.)
Maybe that helps you too
Greetings from Peru
Ragon
Hendrik Vogt, 2023/01/20 10:54
Dear Robert,
for a subset K of the graph I consider as the boundary all the vertices that are outside of K but connected to K by an edge. For me, this helps a lot with the intuition.
Best wishes, Hendrik
Johannes Stojanow, 2022/12/06 10:18
Dear virtual lecturers,
it seems to me that some references on lecture 7 are misdirecting. In particular:
P.84 at the end of the second paragraph of the proof, Proposition 5.2 b) is being cited, which does not exist. We only have Lemma 5.2 without enumerated items.
P.84 at the beginning of the third paragraph, Proposition 5.2 c) is being cited, which does not exist either.
P.86 after the proof of (b), we cite Lemma 5.2 c), while Lemma 5.2 has no enumerated items.
P.86 right below remark 5.5, Lemma 5.2 b) is being cited.
P.87 on the first line, Lemma 5.2 b) again.
I'm guessing, that Lemma 5.2 on domain monotonicity covers the statement of lost Lemma 5.2 c), while b) covers the Markov property. What could have been Lemma 5.2 a) then?
Best regards,
Johannes
Christian Seifert, 2022/12/06 12:07
Dear Johannes,
Many thanks; indeed, there is something wrong here. The Markov property for the restrictions to finite subsets is stated in the paragraph before Lemma 5.2, Proposition 5.2 is Lemma 5.2 (without enumerations).
We will update the text accordingly.
Best,
Christian
Christian Seifert, 2022/12/05 08:33
Dear Paco,
You can of course send your solutions to us by e-mail. We will check them briefly and then publish them on the web page.
Best,
Christian
Francisco Ezquerra Larrodé, 2022/12/07 16:16
Thank you, Christian. Much appreciated.
Francisco Ezquerra Larrodé, 2022/12/03 14:27
Dear Authors,
In team Hagen, we are solving at least two of the exercises proposed for each lecture each week.
Would be OK if we post our solutions to the exercises for previous lectures? This is a unique opportunity to receive feedback, see different solution methods, and we could also help the teams responsible for the exercises . (Currently, only the exercises for Lecture 1 have been posted. )
What do you think?
Best Regards,
Paco
discussion/lecture07.txt · Last modified: 2022/11/15 18:10 by matcs
Discussion on Lecture 07
Dear all,
regarding the last step in the proof of Lemma 5.8, namely the convergence un→u, isn't this just the usual argument that Bnfn→Bf for a sequence (Bn) of operators between to Banach spaces that converges strongly to B and a sequence fn that converges to f in the norm of the first Banach space?
Best wishes, Hendrik
Dear Hendrik,
Many thanks. Yes, this is indeed the abstract argument.
Best, Christian
Dear Chistian,
thanks for the feedback!
Best wishes, Hendrik
Hello,
In Lemma 5.9 we talk about a w0 but it is nowhere defined, should that be a w?
Greetings Ragon
Hi Ragon,
It seems to me that w0 is the initial condition for the supersolution w, i.e. w0=w(0).
Cheers, Jonathan
Dear Ragon and Jonathan,
Yes, w0 is the initial condition of w.
Best, Christian
Dear authors,
in the proof of the Theorem 5.15 (i′)⇒(ii) shouldnt the contraction C[0,1α] used instead of C[0,α]?
Best, Anna
Dear Anna,
Many thanks; you are absolutely right.
Best, Christian
Dear all,
I have a small question concerning Theorem 5.15. In condition (ii), is “for every” equivalent to “for some” α>0?
Regards, Sahiba
Dear ISEM-Team,
I have a question concerning Exercise 7.1: Shouldn't we assume that c=0? Otherwise the statement seems to be wrong (just consider X={x} to be a singleton and c(x)=1).
Best regards
Sascha
Dear Sascha,
Many thanks. Indeed, we should assume c=0 there.
Best, Christian
Dear virtual lecturers,
in the discussions in the Darmstadt team we found several times that what we are truly missing is some sort of reference example of a graph, that helps to see the effects described in the text. In particular the behavior of solutions to the heat equation should be something that has an obvious physical intuition and it would be nice to see this in some concrete example.
I try to explain what I mean: I always try to compare the results with the situation in spatial domains that I know better and there for instance the domain monotonicity described in this lecture is something completely intuitive and it becomes also clear there why it only works for Dirichlet boundary conditions and not for Neumann conditions. I am still lacking an intuition what the “boundary conditions” mean here, as there is no apparent boundary in the graphs and I would hope to see the difference of these boundary conditions in a concrete example. Is something like this possible and will there be some examples in future lectures?
Finally one remark about the text of lecture 7: In the proof of Lemma 5.3 (b) (line 22 ff of page 85) you want to show that x↦e−tx belongs to A for all t≥0. As you later prove that A equals C0([0,∞)) that cannot be true for t=0, as then this function is constantly one and thus does not belong to this space. In fact you probably mean that the assertion of the Lemma is obvious for t=0 and the argument given gives the assertion for all t>0.
Best regards,
Robert
Dear Robert,
Many thanks for the comment and remark.
Indeed, we will provide some class of examples in the last lecture.
Best, Christian
Hello Robert,
It helped me a lot to work through the examples and applications which are given in Chapter 0 in the book. Especially in Chapter 0.4 and 0.5. Also there are special Example exercises for classic graphs (star graphs, line graphs etc.) Maybe that helps you too
Greetings from Peru Ragon
Dear Robert,
for a subset K of the graph I consider as the boundary all the vertices that are outside of K but connected to K by an edge. For me, this helps a lot with the intuition.
Best wishes, Hendrik
Dear virtual lecturers,
it seems to me that some references on lecture 7 are misdirecting. In particular:
I'm guessing, that Lemma 5.2 on domain monotonicity covers the statement of lost Lemma 5.2 c), while b) covers the Markov property. What could have been Lemma 5.2 a) then?
Best regards, Johannes
Dear Johannes,
Many thanks; indeed, there is something wrong here. The Markov property for the restrictions to finite subsets is stated in the paragraph before Lemma 5.2, Proposition 5.2 is Lemma 5.2 (without enumerations).
We will update the text accordingly.
Best, Christian
Dear Paco,
You can of course send your solutions to us by e-mail. We will check them briefly and then publish them on the web page.
Best, Christian
Thank you, Christian. Much appreciated.
Dear Authors,
In team Hagen, we are solving at least two of the exercises proposed for each lecture each week.
Would be OK if we post our solutions to the exercises for previous lectures? This is a unique opportunity to receive feedback, see different solution methods, and we could also help the teams responsible for the exercises
. (Currently, only the exercises for Lecture 1 have been posted. )
What do you think?
Best Regards,
Paco