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STEP 2013 Solutions

Unofficial STEP Solutions 2013

Here is a thread of all of the STEP Solutions (I, II and III) that have been created by TSR users. I will update (or the relevant mod) when new solutions are posted :smile:

STEP I (Sat 25th June 2013)

Question 1: cpdavis
Question 2: mikelbird
Question 3: FJacob
Question 4: Pyoro, cpdavis
Question 5: mikelbird
Question 6: mikelbird
Question 7: Mastermind2
Question 8: metaltron
Question 9: DJMayes
Question 10: DJMayes
Question 11: DJMayes
Question 12: HCIO
Question 13: DFranklin

STEP II (Sat 19th June 2013)

Question 1: mikelbird
Question 2: Smaug123 Alternative to part ii - Fuzzy12345
Question 3: mikelbird Part ii without considering turning points: Nebula
Question 4: jack.hadamard
Question 5: cpdavis
Question 6: metaltron
Question 7: DJMayes
Question 8:MW24595
Question 9: LShirley95
Question 10: DJMayes
Question 11: DJMayes
Question 12: Smaug123
Question 13: Nebula

STEP III (Sat 26th June 2013)

Question 1: Pyoro
Question 2: borealis72
Question 3: jack.hadamard
Question 4: IrrationalNumber, Blutooth
Question 5: jack.hadamard
Question 6: jack.hadamard
Question 7: DJMayes
Question 8: jack.hadamard
Question 9: Brammer
Question 10: DJMayes
Question 11: bananarama2
Question 12: Blutooth, ukdragon37 - only part iic, MAD Phil
Question 13: DFranklin

STEP I Paper: http://www.thestudentroom.co.uk/showpost.php?p=43320667&postcount=1205
STEP II Paper: http://www.thestudentroom.co.uk/showpost.php?p=43252399&postcount=671
STEP III Paper: http://www.thestudentroom.co.uk/showpost.php?p=43334052&postcount=1384
(edited 9 years ago)

Scroll to see replies

Reply 1
You wouldn't happen to have the full paper would you? :tongue:
Reply 2
Original post by LShirley95
You wouldn't happen to have the full paper would you? :tongue:


Yep, thanks Jack! http://www.thestudentroom.co.uk/showpost.php?p=43252399&postcount=672
Reply 3
Question 2:

Spoiler

(edited 10 years ago)
Alternatively to Q2 ii

Spoiler

(edited 10 years ago)
Q7 STEP II

Part i):

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Part ii):

Spoiler



Part iii):

Spoiler

(edited 10 years ago)
Q10 - STEP II:

Part i):

Spoiler



Part ii):

Spoiler



Part iii):

Spoiler

Q11 STEP II
Part i):

Spoiler



Part ii):

Spoiler

(edited 10 years ago)
Reply 8
Got Q9 written with diagrams, unfortunately don't have a scanner so this is the best I can do:
1371760817848.jpg
1371760837517.jpg
1371760848354.jpg

Posted from TSR Mobile
Reply 9
In case anyone wants a higher res version of the (II) paper to work from:

http://www.thestudentroom.co.uk/showpost.php?p=43258896&postcount=829
Reply 10
13 (i)

Spoiler


13 (ii)

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13 (iii)

Spoiler



Alternate to 3ii without considering turning points:

Spoiler

(edited 10 years ago)
Reply 11
Q12:

i)

Spoiler



ii)

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Expression for Var(Y):

Spoiler



Do non-zero λ\lambda exist?

Spoiler

(edited 10 years ago)
Question 6:

Part i)

Spoiler



ii)

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iii)

Spoiler

(edited 10 years ago)
Reply 13
Original post by Smaug123
Q12:

i)

Spoiler



ii)

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Expression for Var(Y):

Spoiler



Do non-zero λ\lambda exist?

Spoiler




I got very similar but ended up having to show that a^2+b^2/(a+b)^2= 1, which of course isn't possible for non zero values. Not sure but think you might have missed out a lambda squared term when cancelling.
Reply 14
Original post by Zorgz
Not sure but think you might have missed out a lambda squared term when cancelling.

Thanks for that - I lost a minus sign and a lambdasquared. Fixed :smile: that's what you get for trying to do it all in LaTeX without using paper first!
Reply 15
Getting ready to type up a solution to question 5 :yep: Also going to update OP
Reply 16
Question 5:

Spoiler

(edited 10 years ago)
Reply 17
Question 8

i- Let A(x,t)A(x, t) be the area of any rectangle with sides parallel to the co-ordinate axes, with one side on y=f(t)y= f(t) and another on the y-axis, and with one corner on the curve f(x). It is clear that, the rectangle with the maximum area will be one of this type.

Looking at a rudimentary diagram, it is evident that:

A(x,t)=x(f(x)f(t))[br][br]dA(x,t)dx=(f(x)f(t))+xf(x)[br] A(x,t)= x(f(x)-f(t))[br][br]\Rightarrow \displaystyle \frac{dA(x,t)}{dx} = (f(x)-f(t)) + x f'(x)[br]

Now, as we're concerned with maximising area, let x0 x_0 be the value of x for which A(x,t) A(x,t) is greatest. So,

dA(x,t)dx=0[br][br](f(x0)f(t))+xf(x0)=0[br][br]x0f(x0)+f(x0)=f(t)[br][br]\displaystyle \frac{dA(x,t)}{dx} = 0[br][br]\Rightarrow (f(x_0)-f(t)) + x f'(x_0) = 0[br][br]\Rightarrow x_0 f'(x_0)+ f(x_0) = f(t)[br][br]

By definition,A0(t) A_0 (t) is the maximum value of A(x,t)A(x,t) so,

A0(t)=x0(f(x0)f(t)) A_0(t) = x_0 (f(x_0)-f(t))

ii- So, we have,

tg(t)=0tf(x) dx[br][br]d(tg(t)dt=ddt(0tf(x) dx)[br][br] tg(t) = \displaystyle \int_0^t f(x)\ dx [br][br]\Rightarrow \frac{d(t g(t)}{dt} = \frac{d}{dt} (\displaystyle \int_0^t f(x)\ dx )[br][br]

Now, notice that on integrating, we have a difference between a function of t and a constant. On differentiating this with respect to t, we just get f(t) f(t) on the RHS. To see this, let h(x)h(x) be the antiderivative of f(x) f(x) .

Then,

tg(t)=h(t)h(0)[br][br]d(tg(t))dt=d(h(t)h(0))dt=dh(t)dt=f(t)[br][br]tg(t)+g(t)=f(t)[br][br]tg(t)=f(t)g(t)[br] tg(t) = h(t) - h(0)[br][br]\Rightarrow \frac{d(t g(t))}{dt} = \frac{d(h(t) - h(0))}{dt} = \frac{d h(t)}{dt} = f(t)[br][br]\Rightarrow t g'(t) + g(t) = f(t)[br][br]\Rightarrow tg'(t) = f(t)- g(t)[br]


Now, consider that:

0t(f(x)f(t)) dx=0x0(f(x)f(t)) dx+x0t(f(x)f(t)) dx \displaystyle \int^t_0 (f(x)-f(t))\ dx = \displaystyle \int^{x_0}_0 (f(x)-f(t))\ dx + \displaystyle \int^t_{x_0} (f(x)-f(t))\ dx

Further, as f(x) f(x) is a decreasing function, we have, for all 0x<x0 0 \le x< x_0 ,

f(x)>f(x0)[br][br]0x0f(x) dx>0x0f(x0) dx=f(x0)0x0 dx=x0f(x0)[br][br]0x0f(x) dxx0(f(t))=x0(f(x0)f(t))[br][br]0x0f(x)f(t) dx=x0(f(x0)f(t))[br][br] f(x) > f(x_0)[br][br]\Rightarrow \displaystyle \int^{x_0}_0 f(x)\ dx > \displaystyle \int^{x_0}_0 f(x_0)\ dx = f(x_0) \displaystyle \int^{x_0}_0\ dx = x_0 f(x_0)[br][br]\Rightarrow \displaystyle \int^{x_0}_0 f(x)\ dx - x_0(f(t)) = x_0 (f(x_0)- f(t))[br][br]\Rightarrow \displaystyle \int^{x_0}_0 f(x)-f(t)\ dx = x_0 (f(x_0)- f(t))[br][br]


Further, for x0x<t x_0 \le x < t , we have,

f(x)>f(t)[br][br]x0tf(x) dx>x0tf(t) dx[br][br]x0tf(x)f(t) dx>0 f(x) > f(t)[br][br]\Rightarrow \displaystyle \int_{x_0}^t f(x)\ dx >\displaystyle \int_{x_0}^t f(t)\ dx[br][br]\Rightarrow \displaystyle \int_{x_0}^t f(x)- f(t)\ dx >0


Therefore, we clearly have,

0x0(f(x)f(t)) dx+x0t(f(x)f(t)) dx>x0(f(x0)f(t))[br][br][br]0t(f(x)f(t)) dx>A0(t)[br][br]\displaystyle \int^{x_0}_0 (f(x)-f(t))\ dx + \displaystyle \int^t_{x_0} (f(x)-f(t))\ dx > x_0 (f(x_0) - f(t))[br][br][br]\Rightarrow \displaystyle \int^t_0 (f(x)-f(t))\ dx > A_0(t)[br][br]

Now, observe that,

Unparseable latex formula:

\displaystyle \int^t_0 (f(x)-f(t))\ dx[br][br]\beginaligned = \displaystyle \int^t_0 f(x)\ dx - t(f(t))[br][br]\beginaligned = t g(t) - t f(t)[br][br]\beginaligned = -t(f(t) - g(t))[br][br]\beginaligned = -t(tg'(t)) = -t^2 g'(t)[br][br]\Rightarrow -t^2 g'(t) >A_0 (t)[br][br]



iii-

f(x)=11+xf(x)=1(1+x)2 f(x) = \frac{1}{1+x} \Rightarrow f'(x) = \frac{-1}{(1+x)^2}

Now, if order to find x0x_0 , we simply plug these into the condition for x0x_0 , namely:

x0f(x0)+f(x0)=f(t)[br][br]x0(1+x0)2+11+x0=11+t[br][br]x0=1+1+t[br][br] x_0 f'(x_0)+ f(x_0) = f(t)[br][br]\Rightarrow \displaystyle \frac{-x_0}{(1+x_0)^2} + \frac{1}{1+x_0} = \frac{1}{1+t}[br][br]\Rightarrow x_0 = -1+ \sqrt {1+t}[br][br]

Now,

g(t)=1t0t11+x dx=1t(ln(1+t))[br][br]tg(t)=f(t)g(t)=11+t1t(ln(1+t))[br][br]t2g(t)=ln(1+t)t1+t[br][br] g(t) = \frac{1}{t} \displaystyle \int_0^t \frac{1}{1+x}\ dx = \frac{1}{t} (ln(1+t))[br][br]\Rightarrow tg'(t) = f(t) - g(t) = \frac{1}{1+t} - \frac{1}{t} (ln(1+t))[br][br]\Rightarrow -t^2 g'(t) = ln(1+t) - \frac{t}{1+t}[br][br]

Similarly, we have,

Unparseable latex formula:

A_0(t) = x_0 (f(x_0) - f(t))[br][br]\beginaligned = \displaystyle (-1+ \sqrt {1+t})(\frac{1}{ \sqrt {1+t}} - \frac{1}{1+t})[br][br]\beginaligned \Rightarrow A_0(t) = 1- \frac{2}{ \sqrt {1+t}} + \frac{1}{1+t}[br][br]



Now, from the previous part's inequality, we get,

t2g0(t)>A0(t)[br][br]ln(1+t)t1+t>121+t+11+t[br][br]ln(1+t)>221+t[br][br]ln1+t>111+t[br][br] -t^2 g_0(t) > A_0(t)[br][br]\Rightarrow ln(1+t) - \frac{t}{1+t} > 1- \frac{2}{ \sqrt {1+t}} + \frac{1}{1+t}[br][br]\Rightarrow ln (1+t) > 2- \frac{2}{ \sqrt {1+t}}[br][br]\Rightarrow ln \sqrt{1+t} > 1- \frac{1}{ \sqrt {1+t}}[br][br]
(edited 10 years ago)
I had to practice some drawing on a software, so enjoy.

Question 4


Preliminary stuff

Spoiler



First part

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Second part (a)

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Second part (b)

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(edited 10 years ago)
Reply 19
Original post by LShirley95
Got Q9 written with diagrams, unfortunately don't have a scanner so this is the best I can do:
1371760817848.jpg
1371760837517.jpg
1371760848354.jpg

Posted from TSR Mobile


How do you figure out the direction for friction? Sorry if you explained it already, but it is hard to read your attachments.

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