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STEP Maths I, II, III 1995 Solutions

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Speleo
STEP III Question 3

(sorry, it was calling to me :tongue:)

No marks for clarity unfortunately.

Aux. quadratic:
m^2 + 2km + 1 = 0
m = [-2k +- sqrt(4k^2 - 4)]/2
m = -k +- sqrt(k^2 - 1)

i) k > 1
x = e^(-kt).[Ae^(sqrt(k^2 - 1)t) + Be^(-sqrt(k^2 - 1)t)]

ii) k = 1
x = (At + B)e^(-kt)

iii) 0 < k < 1
x = e^(-kt).[Acos(sqrt(k^2 - 1)t) + Bsin(sqrt(k^2 - 1)t)]

x(0) = 0
0 = A
x = Be^(-kt)sin(sqrt(k^2-1)t)

dx/dt = -kBe^(-kt)sin(sqrt(k^2-1)t) + sqrt(k^2-1)Be^(-kt)cos(sqrt(k^2-1)t) = 0 at max/min.
ksin(sqrt(k^2-1)t) = sqrt(k^2-1)cos(sqrt(k^2-1)t)
tan(sqrt(k^2-1)t) = sqrt(k^2-1)/k
sqrt(k^2-1)t = arctan[sqrt(k^2-1)/k] + mpi
t = [1/sqrt(k^2-1)]arctan[sqrt(k^2-1)/k] + mpi/sqrt(k^2-1)

When dividing successive x terms, the difference in the e term will just be pi/sqrt(k^2-1).
x_n+1/x_n = e^(-kpi/sqrt(k^2-1)) sin[arctan[sqrt(k^2-1)/k] + (m+1)pi]/sin[arctan[sqrt(k^2-1)/k] + mpi]
sin(t + pi) = -sinpi
x_n+1/x_n = -e^(-kpi/sqrt(k^2-1))
e^(-kpi/sqrt(k^2-1)) = a.
-kpi/sqrt(k^2-1) = lna
k^2/(k^2-1) = (lna)^2/(pi)^2
k^2 = k^2(lna)^2/(pi)^2 - (lna)^2/(pi)^2
k^2((lna)^2/(pi)^2 - 1) = (lna)^2/(pi)^2
k^2[((lna)^2 - (pi)^2)/(pi)^2] = (lna)^2/(pi)^2
k^2 = (lna)^2/[(pi)^2 + (lna)^2



Unless i'm missing something here or am just too tired to function properly, doesn't the second to last line....

k^2[((lna)^2 - (pi)^2)/(pi)^2] = (lna)^2/(pi)^2

imply that the final solution is....

k^2 = (lna)^2/[(pi)^2 - (lna)^2]

Which would be the wrong answer, but i agree with everything else you've done up until that point so i don't know what's up with this final bit.
maltodextrin
Unless i'm missing something here or am just too tired to function properly, doesn't the second to last line....

k^2[((lna)^2 - (pi)^2)/(pi)^2] = (lna)^2/(pi)^2

imply that the final solution is....

k^2 = (lna)^2/[(pi)^2 - (lna)^2]

Which would be the wrong answer, but i agree with everything else you've done up until that point so i don't know what's up with this final bit.
OK, there's a mistake quite early on in what Speleo's done that follows through everywhere and I think is causing the -ve sign.

We're in the 0 < k < 1 case, and so we want ekxsinx1k2e^{-kx} \sin x\sqrt{1-k^2}, not ekxsinxk21e^{-kx} \sin x\sqrt{k^2-1}.
DFranklin
OK, there's a mistake quite early on in what Speleo's done that follows through everywhere and I think is causing the -ve sign.

We're in the 0 < k < 1 case, and so we want ekxsinx1k2e^{-kx} \sin x\sqrt{1-k^2}, not ekxsinxk21e^{-kx} \sin x\sqrt{k^2-1}.


Thanks!
DFranklin
STEP II, 1995, Q2:

Of course, there's nothing special about painting the first post red (as opposed to blue or white), so the number of ways of painting n+1 posts so no two posts are the same colour and the first and last posts are coloured the same is just 3 times what we've just calculated. But then by identifying the 1st and last posts (which are the same colour), we are left with the same situation as n posts in a circle. (e.g. if we consider n=13, then we can think of having posts 1,2,...,12 as the hours on a clock, and we consider post 13 to be the same as post 1).

So the required answer is just 3rn+1=2n+2(1)n3r_{n+1} = 2^n+2(-1)^n.

Edit: Mistake spotted by DVS.


That argument is neat, I said that if we paint n posts in a circle and the 'first' post is red, then the 'last' (adjacent) post must be a colour other than red so we'd have tn=snt_{n} = s_{n}, but as the 'first' post needn't be red, we have tn=3snt_{n} = 3s_{n}. Using sn=2n1rns_{n} = 2^{n-1} - r_{n}, the same result follows quickly. I prefer your argument but I kind of like mine too.
1995 II Question 9

First part
Assuming unit density, λ>0\lambda > 0 and measuring x\overline{x} to be the centre of mass originating from the centre of the base of the hemisphere to the direction of the apex of the cone, we have:

mC=13πa2λam_C = \frac{1}{3}\pi a^2\lambda a

mH=23πa3m_H = \frac{2}{3}\pi a^3

(mH+mC)x=3a8mH+λa4mC\displaystyle (m_H+m_C)\overline{x} = -\frac{3a}{8}m_H+\frac{\lambda a}{4}m_C

And so π3(2a3+λa3)x=π3(3a44+λ2a44)    (8+4λ)x=3a+λ2a\displaystyle \frac{\pi}{3}(2a^3 +\lambda a^3)\overline{x} = \frac{\pi}{3}\left(-\frac{3a^4}{4} + \frac{\lambda^2a^4}{4}\right) \iff (8+4\lambda)\overline{x} = -3a+\lambda^2 a (*)

If x>0\overline{x}>0, then the toy will overbalance, and if x<0\overline{x}<0, the toy will always balance. So we have 3+λ2>0    λ>3-3+\lambda^2 >0 \iff \lambda > \sqrt{3} and 3+λ2<0    λ<3-3+\lambda^2 <0 \iff \lambda < \sqrt{3} respectively, as required.

Second part
Now, let's assume that x\overline{x} is measured to be positive going to the opposite direction of the apex of the cone.

When the toy is placed as described, let angle of the horizontal to the line of symmetry be θ\theta. For the toy to be unstable, the centre of mass must be horizontally to the side of the hemisphere to the perpendicular from the edge connecting the hemisphere and the cone. The condition for stability thus is x=a(3λ2)4(2+λ)<arctanθ=aλ    λ(3λ2)<4(2+λ)\displaystyle \overline{x} = \frac{a(3-\lambda^2)}{4(2+\lambda)} <\arctan{\theta} = \frac{a}{\lambda}\iff \lambda(3-\lambda^2)<4(2+\lambda) . Drawing graphs of LHS and RHS of the inequality, we can see that the condition is always true for all values of λ>0\lambda>0.
insparato
Writing out STEP III Question 2 now.

In=0axn+12(ax)12\displaystyle I_n = \int_0^a x^{n+\frac{1}{2}}(a-x)^{\frac{1}{2}}

I0=0ax12(ax)12\displaystyle I_0 = \int_0^a x^{\frac{1}{2}}(a-x)^{\frac{1}{2}}

x=asin2u x = asin^2u

dxdu=2asinucosu \frac{dx}{du} = 2asinucosu

dx=2asinucosu.du dx = 2asinucosu. du

a=asin2u a = asin^2u

u=π2 u = \frac{\pi}{2}

0=asin2u 0 = asin^2u

u=0 u = 0

I0=0π2a12sinu(a12cosu).2asinucosu.du\displaystyle I_0 = \int_0^{\frac{\pi}{2}} a^{\frac{1}{2}}sinu(a^{\frac{1}{2}}cosu).2asinucosu. du

=2a20π2sin2ucos2u\displaystyle = 2a^2\int_0^{\frac{\pi}{2}} sin^2ucos^2u

=2a20π214(1cos2u)(1+cos2u)\displaystyle = 2a^2\int_0^{\frac{\pi}{2}} \frac{1}{4}(1-cos2u)(1+cos2u)

=a220π21cos22u\displaystyle = \frac{a^2}{2} \int_0^{\frac{\pi}{2}} 1-cos^22u

=a220π2112(1cos4u)\displaystyle = \frac{a^2}{2} \int_0^{\frac{\pi}{2}} 1-\frac{1}{2}(1-cos4u)

=a220π21212cos4u\displaystyle = \frac{a^2}{2} \int_0^{\frac{\pi}{2}} \frac{1}{2}-\frac{1}{2}cos4u

=a22[12u18sin4u]0π2 = \frac{a^2}{2} [\frac{1}{2}u - \frac{1}{8}sin4u]_0^{\frac{\pi}{2}}

=a22([π40][00]) = \frac{a^2}{2} ([\frac{\pi}{4} - 0]-[0-0])

=πa28 = \frac{\pi a^2}{8}

ii)
In=0axn+12(ax)12\displaystyle I_n = \int_0^a x^{n+\frac{1}{2}}(a-x)^{\frac{1}{2}}

u=xn+12 u = x^{n+\frac{1}{2}}

dudx=(n+12)xn12 \frac{du}{dx} = (n+\frac{1}{2})x^{n-\frac{1}{2}}

dvdx=(ax)12 \frac{dv}{dx} = (a-x)^{\frac{1}{2}}

v=23(ax)32 v = -\frac{2}{3}(a-x)^{\frac{3}{2}}

Unparseable latex formula:

\displaystyle I_n = [-\frac{2}{3}x^{n+\frac{1}{2}}}(a-x)^{\frac{3}{2}}]_0^a - \int_0^a -\frac{2}{3}(a-x)^{\frac{3}{2}.(n+\frac{1}{2}x^{n-\frac{1}{2}}



In=23(n+12)(ax)32xn12\displaystyle I_n = \frac{2}{3}(n+\frac{1}{2})\int (a-x)^{\frac{3}{2}}x^{n-\frac{1}{2}}

Unparseable latex formula:

\displaystyle I_n = \frac{2}{3}(n+\frac{1}{2})\int (a-x)(a-x)^{\frac{1}{2}x^{n-\frac{1}{2}}



Unparseable latex formula:

\displaystyle I_n = \frac{2}{3}(n+\frac{1}{2})\int a(a-x)^{\frac{1}{2}x^{n-\frac{1}{2}}-(a-x)^{\frac{1}{2}}x^{n+\frac{1}{2}}



In=23(n+12)[aIn1In] I_n = \frac{2}{3}(n+\frac{1}{2})[aI_{n-1} - I_n]

3In=(2n+1)(aIn1In) 3I_n = (2n+1)(aI_{n-1}-I_n)

3In=2anIn12nInIn+aIn1 3I_n = 2anI_{n-1} - 2nI_n -I_n + aI_{n-1}

(2n+4)In=a(2n+1)In1 (2n+4)I_n = a(2n+1)I_{n-1}

In=a(2n+1)2n+4In1 I_n = \frac{a(2n+1)}{2n+4}I_{n-1}


To finish off (it says evaulate In):

In=(2n+1)×(2n1)×....×5×3(2n+4)×(2n+2)×....×8×6anI0=(2n+1)!πan+222n+4n!(n+2)! \\ I_n = \frac{(2n+1)\times(2n-1)\times....\times5\times3}{(2n+4)\times(2n+2)\times....\times8\times6}a^nI_0 = \frac{(2n+1)!\pi a^{n+2}}{2^{2n+4}n!(n+2)!}

Could someone please check this, I may have made a little mistake somewhere.

P.S. If anyone can explain that "es" I'd love to here it, if I hover it shows I have "\tim es" but in fact I have "\times". Any ideas?
Speleo
STEP III Question 4[spolier]

Cn(t)sin(1/2)t = cos(0)tsin(1/2)t + cos(1)tsin(1/2)t + cos(2)tsin(1/2)t + ... + cos(n)tsin(1/2)t
= (1/2)[2sin(1/2)t + sin(3/2)t - sin(1/2)t + sin(5/2)t - sin(3/2)t + ... + sin(n + 1/2)t]
= (1/2)[sin(1/2)t + sin(n+ 1/2)t]
= sin[(n+1)/2]t.cos[n/2]t
Cn(t) = sin[(n+1)/2]t.cos[n/2]t/sin(1/2)t
as required.

Sn(t)sin(1/2)t = sin(0)t.sin(1/2)t + sin(1)t.sin(1/2)t + sin(2)t.sin(1/2)t + ... + sin(n)tsin(1/2)t
= (1/2)[cos(3/2)t - cos(1/2)t + cos(5/2)t - cos(3/2)t + ... + cos[n+ 1/2]t]
= (1/2)[cos[(n+ 1/2]t - cos(1/2)t]
= sin[(n+1)/2]t.sin[n/2]t
Sn(t) = sin[(n+1)/2]t.sin[n/2]t/sin(1/2)t

Cn(t) - (1/2) = sin[(n+1)/2]t.cos[n/2]t/sin(1/2)t - 1/2
= {2sin[(n+1)/2]t.cos[n/2]t - sin(1/2)t}/2sin(1/2)t
|Cn(t) - (1/2)| = |{2sin[(n+1)/2]t.cos[n/2]t - sin(1/2)t}/2sin(1/2)t|
But 0 < t < 2pi, so sin(1/2)t > 0
So:
|Cn(t) - (1/2)| = |2sin[(n+1)/2]t.cos[n/2]t - sin(1/2)t|/2sin(1/2)t
Consider the expression in the modulus signs on the RHS of the equation:
2sin[(n+1)/2]t.cos[n/2]t - sin(1/2)t
= sin(n + 1/2)t + sin(1/2)t - sin(1/2)t
= sin(n + 1/2)t
|sin(n+ 1/2)t| <= 1

So:

|Cn(t) - (1/2)| <= 1/[2sin(1/2)t]


This question is extremely difficult when you have never encountered the sin/cos addition formulae other than at a glance in the formula book - I did the first part by induction then had no idea what to do for sin so guessed until I found something I could prove by induction - nasty!

Why do I always pick strange ways of doing problems? :confused:

By the way, if you want to practice induction, this would be a good one.
Reply 107
STEP I, Question 14

Spoiler



σ2=pqn\sigma^2 = \frac{pq}{n}

pepσnN(0,12)\frac{p_e - p}{\frac{\sigma}{\sqrt{n}}} \sim N(0,1^2)

So we want 2.5758×pqn<0.012.5758 \times \frac{\sqrt{pq}}{n} < 0.01

Take p=12p = \frac{1}{2}, worst case scenario and reasonable for the proportion of women

So n129n \ge 129

Since pq\sqrt{pq} will decrease, we can take a smaller sample for millionaires over lefties
Reply 108
Should the answer to 1995 STEP I Q12 (i) be 2 times the answer given since the 2 hockey pupils at each end can swap places?
SimonM
STEP I Question 12

Part (i)

Spoiler


Part (ii)

Spoiler


Part (iii)[spoiler]Line up our non-hockey players. They leave (n-r+1) "slots" to put hockey players in (one player per slot). We can arrange this in (nr+1r)×r!\binom{n-r+1}{r} \times r! ways. Therefore our probability is:

(nr+1r)r!n!=(nr+1)!r!n!r!(nr+1r)!=(nr+1)!n!(n2r+1)!\displaystyle \frac{\binom{n-r+1}{r} r!}{n!} = \frac{(n-r+1)!r!}{n!r!(n-r+1-r)!} = \boxed{\frac{(n-r+1)!}{n!(n-2r+1)!}}



(iii) Shouldn't we also take into account the (n-r)! ways of arranging the hockey players in their positions?
SimonM
STEP I, Question 14

Spoiler



σ2=pqn\sigma^2 = \frac{pq}{n}

Unparseable latex formula:

\frac{p_e - p}{\frac{\sigma}{\sqrt{n}} \sim N(0,1^2)



So we want 2.5758×pqn<0.012.5758 \times \frac{\sqrt{pq}}{n} < 0.01

Take p=12p = \frac{1}{2}, worst case scenario and reasonable for the proportion of women

So n129n \ge 129

Since pq\sqrt{pq} will decrease, we can take a smaller sample for millionaires over lefties


Shouldn't the n be inside the square root?
Reply 111
insparato
Having a go at STEP I Question 3 now.

3 i)

Sum of Differences method

f(r) - f(r-1) = .....

f(1) - f(0)
f(2) - f(1)
f(3) - f(2)
.
.
.
f(n-1) - f(n-2)
f(n) - f(n-1)

All terms cancel except two f(n) and f(0)

Therefore

r=1nf(r)f(r1)=f(n)f(0)\displaystyle \sum_{r=1}^n f(r) - f(r-1) = f(n) - f(0)

ii) f(r)=r2(r+1)2 f(r) = r^2(r+1)^2

f(r1)=r2(r1)2 f(r-1) = r^2(r-1)^2

f(r)f(r1)=r2(r+1)2r2(r1)2 f(r) - f(r-1) = r^2(r+1)^2 - r^2(r-1)^2

=r2(r2+2r+1r2+2r1)=4r3 = r^2(r^2+2r+1 -r^2+2r-1) = 4r^3

Therefore

r=1nf(r)f(r1)=f(n)f(0)=n2(n+1)2\displaystyle \sum_{r=1}^n f(r) - f(r-1) = f(n) - f(0) = n^2(n+1)^2

r=1nf(r)f(r1)=r=1n4r3=n2(n+1)2\displaystyle \sum_{r=1}^n f(r)-f(r-1) = \sum_{r=1}^n 4r^3 = n^2(n+1)^2

r=1nr3=14n2(n+1)2\displaystyle \sum_{r=1}^n r^3 = \frac{1}{4}n^2(n+1)^2

iii)

r=1n(2n1)3r=1n(2n)3\displaystyle \sum_{r=1}^n (2n-1)^3 - \sum_{r=1}^n (2n)^3

14(2n1)2(2n)214(2n)2(2n+1)2 \frac{1}{4}(2n-1)^2(2n)^2 - \frac{1}{4}(2n)^2(2n+1)^2

n2(4n24n+1(4n2+4n+1)) n^2(4n^2-4n+1 -(4n^2+4n+1))

n2(8n) n^2(-8n)

8n3 -8n^3

Hmm ive gone wrong somewhere on the last part.

Oh looking at the paper 1^3 - 2^3 + 3^3 .......(2n+1)^3 hmmm where does (2n+1)^3

surely sum (2n-1)^3 - sum(2n)^3 should work ?


For the last part:
Let Sn=RHS
Sn-1= 3^3-2^3+5^3-4^3......
= Sum from n=1 to n=n of (2n+1)^3 - (2n)^3
= Sum 1 to n of[12n^2+6n+1]
= 2n(n+1)(2n+1)+3n(n+1)+n
=n(2(2nn+3n+1)+(3n+3)+1)
=n(4nn+9n+6)

Hence Sn=n(4nn+9n+6) + 1


Speleo
STEP I Question 6

i) y^-2.dy/dx + y^-1 = e^2x
Let u = 1/y
du/dy = -y^-2
dy/dx = du/dx.dy/du = -y^2.du/dx = -u^-2.du/dx
-du/dx + u = e^2x
du/dx - u = -e^2x
(e^-x)du/dx - (e^-x)u = -e^(x)
d/dx(ue^-x) = -e^x
ue^-x = A - e^x
u = Ae^x - e^2x
y = 1/[Ae^x - e^2x]

ii) y^-3.dy/dx + y^-2 = e^2x
Let u = y^-2
du/dy = -2y^-3
dy/dx = du/dx.dy/du = du/dx.-(1/2)y^3
= -(1/2)u^(-3/2).du/dx
-(1/2)u^(3/2)u^(-3/2).du/dx + u = e^2x
du/dx - 2u = -2e^2x
(e^-2x)du/dx - (e^-2x)u = -2
d/dx[ue^-2x] = -2

ue^-2x = B - 2x
u = Be^2x - 2xe^2x
y = 1/sqrt[Be^2x - 2xe^2x]


Looking at this:
(e^-2x)du/dx - (e^-2x)u = -2
d/dx[ue^-2x] = -2

d[ue^-2x]/dx= (e^-2x)du/dx - 2ue^(-2x) =/= (e^-2x)du/dx - (e^-2x)u
Reply 112
Am I being completely retarded, or is there a slight mistake in question 7 in STEP II? There's a 1/16 missing on the equation under 'Now use the formula a^2 = b^2 + c^2 - 2bcCosA).
refref
Am I being completely retarded, or is there a slight mistake in question 7 in STEP II? There's a 1/16 missing on the equation under 'Now use the formula a^2 = b^2 + c^2 - 2bcCosA).

Yeah, in my copy of it there's a "letter to supervisors" saying about the mistake
Reply 114
matt2k8
Yeah, in my copy of it there's a "letter to supervisors" saying about the mistake


Thanks. When doing the question I was looking for a way to get rid of that 1/16 :frown:
Reply 115
STEP II Q3

For the table, I decided to just do it by score each race because it's more natural then position. So the final answer, Where did Barthes come in the final stage, is last.

Also, I hope I haven't missed something by assuming 'dismal' is a codeword for last place.

Finally, any criticism is welcome because i'm not sure what their willing to accept.

edit: I just did Q7 too, except for the factorising part in the middle of (ii) I just assumed it's true iff etc. untill both sides were obviously the same. Is this exceptable, and in any case can anyone tip me on how to factorise such expressions (if it wasn't a 'show this' then I wouldn't have been able to do this)?
Reply 116
Messy, better then nothing.

edit:redface:ops, this is Q6.
Reply 117
It looks like nobody has fixed the front page links in awhile, but according to my computer, whenever I click the answer for STEP I Q 1, it links me to Insperato's answer for Q3. Probably just a hyperlink thing? If not, then has that question been done?
Reply 118
Firago
It looks like nobody has fixed the front page links in awhile, but according to my computer, whenever I click the answer for STEP I Q 1, it links me to Insperato's answer for Q3. Probably just a hyperlink thing? If not, then has that question been done?

Post #17
Reply 119
SimonM


Solution by jj193

STEP I - Q11

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