as such, you can turn one such solution into another solution by replacing x->x+a for any value of $a$. since $a$ can be any real number, there's an infinite number of such transformations and they're all parametrized by the set of allowed $a$
so that set of transformations on solutions actually forms a group
One way to appreciate their use with diff eq's is to think of Lie symmetries as special continuous coordinate transformations which transform one differential equation into an equivalent (but hopefully simpler) differential equation which can more easily be solved
that's not to say it's irrelevant, but it's off the beaten track for most mathematicians. they'd certainly be aware of it, but I'm not sure how much they'd specifically kno about it
for instance, the example I gave above for y'=f(y) can be summed up as: Suppose i have a solution curve for that ode. then if I slide it to the right or left, then that's another solution curve. so the set of solution curves is invariant under horizontal translations
by contrast, if you had y'=f(x) then it'd be invariant under vertical translations
with more complicated odes, it's not at all obvious what sorts of invariance is possible. but if you can find it, then your life becomes a lot easier
When telescopes listen for radio waves far into the galaxy, how do they target exactly that place? I mean, aren't there other RF waves interfering. Also, when you aim the telescope at a planet, how do you know that the RF signal is actually from there and is not something else that has bounced of and so on...?
@bolbteppa Those are excellent text for my level. It has explained symmetry very well by saying “symmetry means changing something so that it is unchanged” (although it doesn’t write that explicitly but I got it that way)