STEP I, II, III 2002 Solutions
Maths exam discussion - share revision tips in preparation for GCSE, A Level and other maths exams and discuss how they went afterwards.
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Re: STEP I, II, III 2002 SolutionsOne of the assumptions for NLR we have for M4 problems is that "collisions are smooth", i.e. the velocity of colliding spheres perpendicular to the line of centres is unchanged. However in this question, velocities perpendicular to the line of centres is changed by the collision.(Original post by ghostwalker)
Unless I'm doing something wrong, NLR doesn't work here, so at least one of the assumptions on which it is based must be invalid in this situation; though to be honest, I've never seen them explicitly stated, just examples where it applies.
The problem shows up most clearly when dealing with the final part of the question, when the angle between the particles after collision is 90 degrees.
If NLR holds here, then, as you stated, the line of centres at collision is in the direction of the velocity of P2. As v1 is perpendicular to this, in this case, it has a zero velocity component along the line of centres, implying it had a zero component along the line of centres prior to the collision, implying the angle phi is 90, and theta is zero, which contradicts the question which states they are non zero.
For what it's worth, I did post a (pretty long) proof of this question at the bottom of the first page.Last edited by Unbounded; 18-06-2010 at 06:48. -
Re: STEP I, II, III 2002 SolutionsCheers, but how do we know this here.(Original post by Unbounded)
One of the assumptions for NLR we have for M4 problems is that "collisions are smooth", i.e. the velocity of colliding spheres perpendicular to the line of centres is unchanged. However in this question, velocities perpendicular to the line of centres is changed by the collision.
Edit: Yep, ignore, I actully showed that myself in my previous post, lol.
Wonder why Simon didn't include it in the solved list in the OP, particularly as it's on the first page. Wish I'd seen it earlier, thanks.For what it's worth, I did post a (pretty long) proof of this question at the bottom of the first page.Last edited by ghostwalker; 18-06-2010 at 07:04. -
Re: STEP I, II, III 2002 Solutions
I'll have to try and draw a proper diagram later, but it's perfectly possible for P1 to have non-zero velocity relative to the line of centers before the collision, and zero velocity afterwards.
In fact that's exactly what you'd expect for a perfectly elastic colliision between two equal masses - as famously demonstrated by a Newton's cradle.
[Of course, since two of you are now questioning that NLR applies here, it's entirely possible I'm talking nonsense].Last edited by DFranklin; 18-06-2010 at 08:43. -
Re: STEP I, II, III 2002 SolutionsYes, I was making the assumption (unconsciously) that P1 was hitting an immoveable object for some unfathomable reason.(Original post by DFranklin)
I'll have to try and draw a proper diagram later, but it's perfectly possible for P1 to have non-zero velocity relative to the line of centers before the collision, and zero velocity afterwards.
Damn. Damn. DAMN!
Back to the drawing board. -
Re: STEP I, II, III 2002 SolutionsImpressively lazy!(Original post by SimonM)
I'm being particularly lazy today, could you link me please?
http://www.thestudentroom.co.uk/show...2&postcount=20
The page for a single post can be found by clicking on the post number at the top of the post.(Original post by ghostwalker)
If I knew how. The format for the links in your OP doesn't match what displays as a URL, so, no can do; sorry. -
Re: STEP I, II, III 2002 Solutions
Using NLR and a couple of momentum equations as detailed below:
Perpendicular to line of "centres":

Parallel to line of centres:

NLR:

and after some nasty algebra (hence I'm not inclined to put the latex in at the moment), I end up with:

Which, whilst reasonably elegant, bears little resemblence to the desired equation.
However, it does still satisfy the requirement that k = 1, when the two paths are perpendicular, which give me some small faith in it.Last edited by ghostwalker; 18-06-2010 at 14:01. -
Re: STEP I, II, III 2002 SolutionsTa, Perhaps I ought to actually read it then. Lol.(Original post by DFranklin)
This line appears in Unbounded's solution, so it does end up in the right place eventually.
Edit: Not too far from the end either. My faith in mechanics is restored and all is right with the world once more. Deep sigh!
Nasty bit of STEPish level work at the end, IMHO. Interestingly, I didn't use the conservation of KE directly in this second one (although implicit in using e=1).
I have to say, of the three solutions, as an impartial observer (not), I prefer my first one.Last edited by ghostwalker; 18-06-2010 at 14:19. -
Re: STEP I, II, III 2002 SolutionsYou disagree then?(Original post by DFranklin)
What was the difference between yours and Unbounded? As described it looked similar, but from what you're saying, his turned out a bit nastier.
Well it avoided the
, avoided the product-sum, seemed, to me, a hell of an lot simpler with the trig manipulations, and really reduced the problem to more standard A-level, rather than STEP, IMHO.
P.S. I did say I was impartial (not)!Last edited by ghostwalker; 18-06-2010 at 14:50. -
Re: STEP I, II, III 2002 Solutions
Wasn't disagreeing, just trying to ascertain where the big "don't do this, do that" point of decision was. It wasn't obvious to me on a cursory glance why your algebra was so much nicer - largely because I wasn't sure what was involved in your "sub (4) into (3) and fiddle" comment. Looking a bit more carefully, I see that there is very little fiddling required, but I didn't notice that at the time.
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Re: STEP I, II, III 2002 Solutions(Original post by DFranklin)
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Yep, "fiddle" with me is a small thing (though someone else may use the term compeletely differently), as opposed to the "after some nasty algebra" in my second solution which involved 8 terms each comprising a combination of three, sines and cosines; yuck!
I guess the main difference was that I didn't square the "momentum in the direction of the initial velocity" equation early on; and later didn't need to.
After stating the initial equations, putting v2 in terms of v1 seemed a natural first step, which would almost certainly come in handy later.
Then "putting (4) into (3) and fiddle" so u is just in terms of v1 produced something akin to the one side of the desired equation (fortuitously perhaps), and the next step was obvious.