Even ignoring manifolds and point set topology you guys can't really ignore field theory & action principles, i.e. classical field theory (
electromagnetism) & the calculus of variations, the way you can ignore manifolds.
If you just jump into GR with a modest background you could ruin the subject for yourself - if you see an action or the EM Lagrangian you can only hope the 5 pages of preparation (if at all) they spent on these was enough, also it'd be pretty awful to start dealing with field tensors without action principles & the theory as a whole would seem pretty divorced from the rest of physics what with all the Riemann's & Christoffel's taking up your time... In other words, the fun naive feeling you have in your head as to what GR is could be totally shattered, you could be left with that awful feeling of confusion, possibly be tricked into thinking that not knowing manifolds and dual spaces is the reason why you're having problems, or just generally have feeling that you can't understand something because you skipped something else that you should have done.
There is a nice way to actually study the structure of GR by studying the prerequisites properly. Look at the table of contents of
Landau vol. 2: chapter's 1 - 9 are SR & EM (
special relativity and electromagnetism) done absolutely from scratch using the (
multi-variable) calculus of variations, 10 - 14 are general relativity. If you look closely you'll notice:
1, 2, 3 ~ 10
4 ~ 11,
5 ~ 12,
6, 7 ~ 13 (
& bits of 9)
That is, chapters 1, 2 & 3 are an easy version of chapter 10, i.e. the structure of GR in chapter 10 closely parallel's what you already did in 1, 2 & 3 taking special relativity and electromagnetism as your example, what you do in chapter 4 is analogous to what you do in chapter 11, etc...
By studying this book you are already studying general relativity on chapter 1, just an easy version of one part of it in such a way that when you get to chapter 10 you'll really appreciate how radical a change GR is in context, you are doing it honestly in a way you won't have to un-learn, developing the necessary prerequisites, & you see the absolute unity of physics at your feet as a by product. No manifolds, no stupid vector calculus EM (
which you don't need to know, better not to tbh), no memorizing Maxwell's equations as if they're god-given or rely on their heuristic derivations, and no need to resort to books like
these.
The only potential roadblocks standing in your way of being able to pick this book up are the (
multi-variable)
calculus of variations and
classical mechanics (
based on single variable calculus of variations), & Landau's hard so you'll probably have to look in other sources at times, but it's always worth more to struggle towards understanding what he's saying than running away, though you might need tools in other books to see it in a nice way, e.g. Noether in Gelfand, Tensor's in
Borisenko, remembering some crazy EM derivations via differential forms in MTW, fun things from
Padmanabhan. Do whatever you have to do but "http://www.researchgate.net/post/Any_recommended_reading_for_physics_undergraduate_student"
Following the above approach is to think of GR as a natural extension of the calculus you know and love, but it is a local approach (
local means you always assume a coordinate system and basis, though arbitrary). Taking the manifolds approach to GR is basically taking the point set topology (
think Kelley) and Lebesgue measure approach to calculus, or at least the metric space & Riemann-Stieltjes approach to real analysis (
still paying lip service to the Kelley & Lebesgue approach) so that you can take a global approach to GR (
global means you don't impose any coordinate system or vector space basis, you do things before laying these out). The benefits are generality, nice global geometric intuition, and more... The cost is that you'll instantly be told to work with a special kind of second-countable Hausdorff topological space out of the blue & to impose conditions that are obvious in, or naturally fall out of, the local approach - if we're going to get so pedantic why not go back to axiomatic set theory and do it properly, taking your time to first do single & multi-variable calculus, using these as practice with your tools so that you'll have some intuition by the time you get to GR? It's chancy to take unfamiliar tools and apply them to something as notoriously difficult as GR when you can do GR using tools you have or are relatively easily accessible. If you didn't do it for calculus, why arbitrarily do it for GR & ignore doing GR in a way you can do based on what you've already done?
To learn GR directly through the language of manifolds without properly developing those tools is to learn a subject unintuitively paying lip service to special cases you have little to no appreciation for while using tools you have little/no intuition for leaving yourself open to committing some basic basic topological error should you stray too far from the path your book sets out. A hint at what you're doing is that you're shifting the emphasis from thinking of your metric as g_{\mu \nu} to thinking of it as g_{\mu \nu} = g(\hat{e}_{\mu},\hat{e}_{\nu}) and giving a set-theoretical & topological foundation to the notion of vectors on a curved surface, what a surface itself is, what it means to define g over the whole surface and then playing a lot of necessary games to do what is very natural using the coordinate approach. There's a lot of value to this approach, but if you didn't have the urge to go back to point set topology in your study of calculus (or axiomatic set theory like I did

) don't think it's absolutely necessary in order to understand GR when it's not.