I'm going to try and do a mark scheme here. Bare in mind that I'm in Year 12 too >.>
Firstly, thanks to Barrel who actually posted the paper (page 15). here are the pages in order:
http://www.thestudentroom.co.uk/attachment.php?attachmentid=426179&d=1434104177 http://www.thestudentroom.co.uk/attachment.php?attachmentid=426181&d=1434104202 http://www.thestudentroom.co.uk/attachment.php?attachmentid=426183&d=1434104269 http://www.thestudentroom.co.uk/attachment.php?attachmentid=426185&d=1434104300 1. y = e 2 x cos x [ b r ] d y d x = e 2 x ( − sin x ) + 2 e 2 x cos x [ b r ] d y d x = e 2 x ( 2 cos x − sin x ) [ 2 ] [ b r ] − s o l v e f o r m a x : [ b r ] 0 = e 2 x ( 2 cos x − sin x ) [ b r ] 2 cos x = sin x [ b r ] tan x = 2 [ 2 ] [ b r ] x = 1.1 t o 2 s . f . [ b r ] − s u b i n t o y = e 2 x cos x [ b r ] y = 4.1 t o 2 s . f . [ b r ] P ( 1.1 , 4.1 ) [ 2 ] 1. \,\, y = e^{2x} \cos x [br]\dfrac{dy}{dx} = e^{2x} (-\sin x) + 2e^{2x} \cos x[br]\dfrac{dy}{dx} = e^{2x} (2 \cos x - \sin x) \,\, [2][br]\mathrm{- solve for max:}[br]0 = e^{2x} (2 \cos x - \sin x) [br]2 \cos x = \sin x [br]\tan x = 2 \,\, [2][br]x = 1.1 \, \mathrm{to 2 s.f.}[br]\mathrm{- sub into y = e^{2x} \cos x}[br]y = 4.1 \, \mathrm{to 2 s.f.} [br]P(1.1, 4.1) \,\, [2] 1. y = e 2 x cos x [ b r ] d x d y = e 2 x ( − sin x ) + 2 e 2 x cos x [ b r ] d x d y = e 2 x ( 2 cos x − sin x ) [ 2 ] [ b r ] − solveformax : [ b r ] 0 = e 2 x ( 2 cos x − sin x ) [ b r ] 2 cos x = sin x [ b r ] tan x = 2 [ 2 ] [ b r ] x = 1.1 to2s.f. [ b r ] − subintoy = e 2x cos x [ b r ] y = 4.1 to2s.f. [ b r ] P ( 1.1 , 4.1 ) [ 2 ] 2. ∫ 2 x − 1 3 d x [ b r ] − s o l v e b y i n s p e c t i o n o f s u b s t i t u t i o n . S u b s t i t u t i o n w o u l d b e u = 2 x − 1 [ b r ] = 3 8 ( 2 x − 1 ) 4 3 + c [ 4 ] 2. \,\, \displaystyle \int \sqrt [3]{2x - 1} \, dx[br]\mathrm{- solve by inspection of substitution. Substitution would be u = 2x - 1}[br]= \dfrac {3}{8} (2x - 1)^{\frac {4}{3}} + c \,\, [4] 2. ∫ 3 2 x − 1 d x [ b r ] − solvebyinspectionofsubstitution.Substitutionwouldbeu = 2x − 1 [ b r ] = 8 3 ( 2 x − 1 ) 3 4 + c [ 4 ] 3. ∫ 1 2 x 3 ln x d x [ b r ] − i n t e g r a t e b y p a r t s : [ b r ] d v d x = x 3 , u = l n x [ b r ] v = x 4 4 , d u d x = 1 x [ 2 ] [ b r ] − f o l l o w t h r o u g h [ 2 ] , a n d [ b r ] = 4 ln 2 − 15 16 [ 1 ] 3. \,\, \displaystyle \int^2 _1 x^{3}\ln x \, dx[br]\mathrm{- integrate by parts:}[br]\dfrac {dv}{dx} = x^{3}, u = lnx[br]v = \dfrac {x^4}{4}, \dfrac{du}{dx} = \frac{1}{x} \,\, [2][br]\mathrm{- follow through [2], and}[br]= 4 \ln 2 - \frac{15}{16} \,\, [1] 3. ∫ 1 2 x 3 ln x d x [ b r ] − integratebyparts : [ b r ] d x d v = x 3 , u = l n x [ b r ] v = 4 x 4 , d x d u = x 1 [ 2 ] [ b r ] − followthrough [ 2 ] , and [ b r ] = 4 ln 2 − 16 15 [ 1 ] 4. V = 1 3 π r 2 h , d V d t = 5 [ b r ] − d r a w a t r i a n g l e : [ b r ] tan 45 = r h [ b r ] r = h [ b r ] V = 1 3 π h 3 [ 2 ] [ b r ] d V d h = π h 2 [ b r ] − c h a i n r u l e : [ b r ] d h d t = d V d t × d h d V = d V d t d V d h [ b r ] d h d t = 5 π h 2 [ 2 ] [ b r ] h = 10 , d h d t = 5 100 π = 1 20 π [ 1 ] 4. \,\, V = \dfrac{1}{3} \pi r^{2} h, \, \dfrac{dV}{dt} = 5[br]\mathrm{- draw a triangle:}[br]\tan 45 = \dfrac{r}{h}[br]r = h[br]V = \dfrac{1}{3} \pi h^3 \,\, [2][br]\dfrac{dV}{dh} = \pi h^2[br]\mathrm{- chain rule:}[br]\dfrac{dh}{dt} = \dfrac{dV}{dt} \times \dfrac{dh}{dV} = \dfrac{\frac{dV}{dt}}{\frac{dV}{dh}}[br]\dfrac{dh}{dt} = \dfrac{5}{\pi h^2} \,\, [2][br]h = 10, \, \dfrac{dh}{dt} = \dfrac{5}{100 \pi} = \dfrac{1}{20 \pi} \,\, [1] 4. V = 3 1 π r 2 h , d t d V = 5 [ b r ] − drawatriangle : [ b r ] tan 45 = h r [ b r ] r = h [ b r ] V = 3 1 π h 3 [ 2 ] [ b r ] d h d V = π h 2 [ b r ] − chainrule : [ b r ] d t d h = d t d V × d V d h = d h d V d t d V [ b r ] d t d h = π h 2 5 [ 2 ] [ b r ] h = 10 , d t d h = 100 π 5 = 20 π 1 [ 1 ] 5. y 2 + 2 x ln y = x 2 [ b r ] − j u s t p u t ( 1 , 1 ) i n − I ′ m n o t w r i t i n g t h a t o u t f o r y o u . . . [ 1 ] [ b r ] − d i f f e r e n t i a t e i m p l i c i t l y : [ b r ] 2 y d y d x + 2 x 1 y d y d x + 2 ln y = 2 x [ b r ] d y d x 2 ( y + x y ) = 2 ( x − ln y ) [ b r ] d y d x = x − ln y y + x y [ 3 ] [ b r ] − s u b s t i t u t e i n ( 1 , 1 ) [ b r ] d y d x = 1 − 0 1 + 1 = 1 2 [ 1 ] 5. \,\, y^2 + 2x \ln y = x^2[br]\mathrm{- just put (1, 1) in - I'm not writing that out for you... [1]}[br]\mathrm{- differentiate implicitly:}[br]2y \dfrac{dy}{dx} + 2x \dfrac{1}{y} \dfrac{dy}{dx} + 2 \ln y = 2x[br]\dfrac{dy}{dx} 2 \left(y + \dfrac{x}{y} \right) = 2 \left(x - \ln y \right)[br]\dfrac{dy}{dx} = \dfrac{x - \ln y}{y + \frac{x}{y}} \,\, [3][br]\mathrm{- substitute in (1, 1)}[br]\dfrac{dy}{dx} = \dfrac{1 - 0}{1 + 1} = \dfrac{1}{2} \, [1] 5. y 2 + 2 x ln y = x 2 [ b r ] − justput ( 1 , 1 ) in − I ′ mnotwritingthatoutforyou... [ 1 ] [ b r ] − differentiateimplicitly : [ b r ] 2 y d x d y + 2 x y 1 d x d y + 2 ln y = 2 x [ b r ] d x d y 2 ( y + y x ) = 2 ( x − ln y ) [ b r ] d x d y = y + y x x − ln y [ 3 ] [ b r ] − substitutein ( 1 , 1 ) [ b r ] d x d y = 1 + 1 1 − 0 = 2 1 [ 1 ] - I wasn't completely sure of the method for the second part, this is what a friend told me the method was (I think I do it correctly). Because of the nature of these two questions, however, I'm not 100% sure you need a method if you get the answer correct. It's only 1 mark each either way ~
6. 6 sin − 1 x − π = 0 [ b r ] sin − 1 x = π 6 [ b r ] x = sin π 6 = 1 2 [ 2 ] [ b r ] m e t h o d : [ b r ] sin − 1 x = cos − 1 x [ b r ] θ = sin − 1 x , θ = cos − 1 x [ b r ] x = sin θ , x = cos θ [ b r ] − d i v i d e t h r o u g h ( s o l v e t h e m s i m u l t a n e o u s l y ) [ b r ] 1 = tan θ [ b r ] θ = π 4 [ b r ] x = sin π 4 = 1 2 ( = 2 2 ) [ 2 ] 6. \,\, 6 \sin ^{-1} x - \pi = 0[br]\sin ^{-1} x = \dfrac{\pi}{6}[br]x = \sin \dfrac{\pi}{6} = \dfrac {1}{2} \,\, [2][br]\mathrm{method:}[br]\sin ^{-1} x = \cos ^{-1} x[br]\theta = \sin ^{-1} x, \, \theta = \cos ^{-1} x[br]x = \sin \theta, \, x = \cos \theta[br]\mathrm{- divide through (solve them simultaneously)}[br]1 = \tan \theta[br]\theta = \dfrac{\pi}{4}[br]x = \sin \dfrac{\pi}{4} = \dfrac{1}{\sqrt{2}} ( = \dfrac{\sqrt{2}}{2}) \,\, [2] 6. 6 sin − 1 x − π = 0 [ b r ] sin − 1 x = 6 π [ b r ] x = sin 6 π = 2 1 [ 2 ] [ b r ] method : [ b r ] sin − 1 x = cos − 1 x [ b r ] θ = sin − 1 x , θ = cos − 1 x [ b r ] x = sin θ , x = cos θ [ b r ] − dividethrough ( solvethemsimultaneously ) [ b r ] 1 = tan θ [ b r ] θ = 4 π [ b r ] x = sin 4 π = 2 1 ( = 2 2 ) [ 2 ] 7. − f o r t h e f i r s t p a r t y o u j u s t s u b s t i t u t e f ( x ) i n w h e r e v e r t h e r e i s a n x i n f ( x ) [ 2 ] [ b r ] − i f y o u r e a l l y w a n t t o s e e i t r e p l y t o t h i s [ b r ] − f o r t h e s e c o n d p a r t , I d i d n ′ t k n o w t h i s a s a n a c t u a l r u l e , b u t : [ b r ] f − 1 ( x ) = f ( x ) [ 1 ] [ b r ] − s u b ( − x ) i n t o g ( x ) , p r o v e t h a t g ( x ) = g ( − x ) , e a s y . [ 2 ] [ b r ] − g ( x ) h a s a l i n e o f s y m m e t r y i n t h e y − a x i s / i s r e f l e c t e d i n t h e y − a x i s o w t t e [ 1 ] 7. \,\, \mathrm{- for \ the \ first \ part \ you \ just \ substitute \ f(x) \ in \ wherever \ there \ is \ an \ x \ in \ f(x) \ [2]}[br]\mathrm{- if you really want to see it reply to this}[br]\mathrm{- for the second part, I didn't know this as an actual rule, but:}[br]f^{-1}(x) = f(x) \,\, [1][br]\mathrm{- sub (-x) into g(x), prove that g(x) = g(-x), easy. [2]}[br]\mathrm{- g(x) has a line of symmetry in the y-axis/is reflected in the y-axis owtte [1]} 7. − for the first part you just substitute f ( x ) in wherever there is an x in f ( x ) [ 2 ] [ b r ] − ifyoureallywanttoseeitreplytothis [ b r ] − forthesecondpart , Idid n ′ tknowthisasanactualrule , but : [ b r ] f − 1 ( x ) = f ( x ) [ 1 ] [ b r ] − sub ( − x ) intog ( x ) , provethatg ( x ) = g ( − x ) , easy. [ 2 ] [ b r ] − g ( x ) hasalineofsymmetryinthey − axis/isreflectedinthey − axisowtte [ 1 ] 8. f ( x ) = ( x − 2 ) 2 x = x 2 − 4 x + 4 x [ b r ] f ( x ) = x − 4 + 4 x − 1 [ b r ] − n o q u o t i e n t r u l e f o r m e , t h a n k s [ b r ] f ′ ( x ) = 1 − 4 x − 2 = 1 − 4 x 2 [ 2 ] [ b r ] f ′ ′ ( x ) = 8 x − 3 = 8 x 3 [ 2 ] [ b r ] − s o l v e f o r Q : [ b r ] 0 = 1 − 4 x 2 [ b r ] 4 x 2 = 1 [ b r ] 4 = x 2 [ b r ] x = ± 2 [ b r ] x = + 2 i s s o l u t i o n f o r P [ b r ] x = − 2 f o r Q [ b r ] f ( − 2 ) = − 8 [ b r ] Q ( − 2 , − 8 ) [ 2 ] [ b r ] f ′ ′ ( − 2 ) = − 1 < 0 s o Q i s a m a x i m u m [ 1 ] 8. \,\, f(x) = \dfrac{(x - 2)^2}{x} = \dfrac{x^2 - 4x + 4}{x}[br]f(x) = x - 4 + 4x^{-1}[br]\mathrm{- no quotient rule for me, thanks}[br]f'(x) = 1 - 4x^{-2} = 1 - \dfrac{4}{x^2} \,\, [2][br]f''(x) = 8x^{-3} = \dfrac{8}{x^3} \,\, [2][br]\mathrm{- solve for Q:}[br]0 = 1 - \dfrac{4}{x^2}[br]\dfrac{4}{x^2} = 1[br]4 = x^2[br]x = \pm 2[br]x = +2 \, \mathrm{is solution for P}[br]x = -2 \, \mathrm{for Q}[br]f(-2) = -8[br]Q(-2, -8) \,\, [2][br]f''(-2) = -1<0 \, \mathrm{so Q is a maximum} \,\, [1] 8. f ( x ) = x ( x − 2 ) 2 = x x 2 − 4 x + 4 [ b r ] f ( x ) = x − 4 + 4 x − 1 [ b r ] − noquotientruleforme , thanks [ b r ] f ′ ( x ) = 1 − 4 x − 2 = 1 − x 2 4 [ 2 ] [ b r ] f ′′ ( x ) = 8 x − 3 = x 3 8 [ 2 ] [ b r ] − solveforQ : [ b r ] 0 = 1 − x 2 4 [ b r ] x 2 4 = 1 [ b r ] 4 = x 2 [ b r ] x = ± 2 [ b r ] x = + 2 issolutionforP [ b r ] x = − 2 forQ [ b r ] f ( − 2 ) = − 8 [ b r ] Q ( − 2 , − 8 ) [ 2 ] [ b r ] f ′′ ( − 2 ) = − 1 < 0 soQisamaximum [ 1 ] − v e r i f y i s s i m p l e [ 2 ] [ b r ] − t h e n e x t p a r t c a n b e d o n e t w o w a y s . . . [ b r ] − r e c t a n g l e − i n t e g r a l : [ b r ] A = 1 × 3 − ∫ 1 4 f ( x ) d x [ b r ] − o r a s a n i n t e g r a l , t o p c u r v e − b o t t o m c u r v e : [ b r ] A = ∫ 1 4 1 − f ( x ) d x [ b r ] − f o l l o w e i t h e r t h r o u g h [ b r ] − t h e i n t e g r a t i o n i s e a s y u s i n g t h e e x p a n s i o n o f f ( x ) [ b r ] A = 15 2 − 4 ln 4 [ 4 ] [ b r ] − n e x t p a r t . . . [ b r ] g ( x ) = f ( x + 1 ) − 1 q e d . [ 3 ] [ b r ] ∫ 0 3 g ( x ) d x = 4 ln 4 − 15 2 [ b r ] = − [ y o u r a n s w e r f r o m b e f o r e ] [ 1 ] [ b r ] − I c a n ′ t r e a l l y s a y w h a t t h e w o r d s f o r t h i s a n s w e r a r e [ 1 ] \mathrm{- \ verify \ is \ simple \ [2]}[br]\mathrm{- the \ next \ part \ can \ be \ done \ two \ ways...}[br]\mathrm{- rectangle - integral:}[br]\displaystyle A = 1 \times 3 - \int ^4 _1 f(x) \, dx[br]\mathrm{- or as an integral, top curve - bottom curve:}[br]\displaystyle A = \int ^4 _1 1 - f(x) \, dx[br]\mathrm{- follow either through}[br]\mathrm{- the integration is easy using the expansion of f(x)}[br]A = \dfrac{15}{2} - 4 \ln 4 \,\, [4][br]\mathrm{- next part...}[br]g(x) = f(x + 1) - 1 \, qed. \,\, [3][br]\displaystyle \int ^3 _0 g(x) \, dx = 4 \ln4 - \dfrac{15}{2}[br]= - \mathrm{[your answer from before]} \,\, [1][br]\mathrm{- I \ can't \ really \ say \ what \ the \ words \ for \ this \ answer \ are} \,\, [1] − verify is simple [ 2 ] [ b r ] − the next part can be done two ways... [ b r ] − rectangle − integral : [ b r ] A = 1 × 3 − ∫ 1 4 f ( x ) d x [ b r ] − orasanintegral , topcurve − bottomcurve : [ b r ] A = ∫ 1 4 1 − f ( x ) d x [ b r ] − followeitherthrough [ b r ] − theintegrationiseasyusingtheexpansionoff ( x ) [ b r ] A = 2 15 − 4 ln 4 [ 4 ] [ b r ] − nextpart... [ b r ] g ( x ) = f ( x + 1 ) − 1 q e d . [ 3 ] [ b r ] ∫ 0 3 g ( x ) d x = 4 ln 4 − 2 15 [ b r ] = − [ youranswerfrombefore ] [ 1 ] [ b r ] − I ca n ′ t really say what the words for this answer are [ 1 ] 9. f ( x ) = ( e x − 2 ) 2 − 1 [ b r ] 0 = ( e x − 2 ) 2 − 1 [ b r ] 1 = ( e x − 2 ) 2 [ b r ] e x − 2 = ± 1 [ b r ] e x = 1 , 3 ( l n 1 i s 0 w h i c h i s f o r O ) [ b r ] x = ln 3 [ 2 ] [ b r ] f ′ ( x ) = 2 e x ( e x − 2 ) [ b r ] 0 = 2 e x ( e x − 2 ) [ b r ] e x = 2 [ b r ] x = ln 2 [ 3 ] [ b r ] f ( ln 2 ) = − 1 [ 1 ] [ b r ] Q ( ln 2 , − 1 ) [ b r ] − a s I s a i d e a r l i e r , i t w a n t s t h e ′ e n c l o s e d ′ a r e a . . . [ b r ] ∫ 0 ln 3 ( e x − 2 ) 2 − 1 d x [ b r ] = ∫ 0 ln 3 e 2 x − 4 e x + 3 d x [ b r ] − f o l l o w t h r o u g h [ 4 ] [ b r ] A = 3 ln 3 − 4 [ 1 ] 9. \,\, f(x) = (e^x - 2)^2 - 1[br]0 = (e^x - 2)^2 - 1[br]1 = (e^x - 2)^2[br]e^x - 2 = \pm 1[br]e^x = 1, 3 \,\, \mathrm{(ln1 \ is \ 0 \ which \ is \ for \ O)}[br]x = \ln 3 \,\, [2][br]f'(x) = 2e^{x} (e^x - 2)[br]0 = 2e^{x} (e^x - 2)[br]e^x = 2[br]x = \ln 2 \,\, [3][br]f(\ln 2) = -1 \,\, [1][br]Q(\ln 2, -1)[br]\mathrm{- as I said earlier, it wants the 'enclosed' area...}[br]\displaystyle \int ^{\ln 3} _0 (e^x - 2)^2 - 1 \, dx[br]\displaystyle= \int ^{\ln 3} _0 e^{2x} - 4e^{x} + 3 \, dx[br]\mathrm{- follow through [4]}[br]A = 3 \ln 3 - 4 \,\, [1] 9. f ( x ) = ( e x − 2 ) 2 − 1 [ b r ] 0 = ( e x − 2 ) 2 − 1 [ b r ] 1 = ( e x − 2 ) 2 [ b r ] e x − 2 = ± 1 [ b r ] e x = 1 , 3 ( ln1 is 0 which is for O ) [ b r ] x = ln 3 [ 2 ] [ b r ] f ′ ( x ) = 2 e x ( e x − 2 ) [ b r ] 0 = 2 e x ( e x − 2 ) [ b r ] e x = 2 [ b r ] x = ln 2 [ 3 ] [ b r ] f ( ln 2 ) = − 1 [ 1 ] [ b r ] Q ( ln 2 , − 1 ) [ b r ] − asIsaidearlier , itwantsth e ′ enclose d ′ area... [ b r ] ∫ 0 l n 3 ( e x − 2 ) 2 − 1 d x [ b r ] = ∫ 0 l n 3 e 2 x − 4 e x + 3 d x [ b r ] − followthrough [ 4 ] [ b r ] A = 3 ln 3 − 4 [ 1 ] − s w a p y a n d x a n d r e a r r a n g e e t c [ b r ] f − 1 ( x ) = ln ( x + 1 + 2 ) [ 3 ] [ b r ] d o m a i n : x ≥ − 1 [ 1 ] [ b r ] r a n g e : f − 1 ( x ) ≥ ln 2 [ 1 ] [ b r ] − g r a p h i s r e f l e c t i o n i n y = x [ 2 ] [ b r ] − s t a r t s a t ( − 1 , l n 2 ) i n t e r c e p t a t l n 3 , t h e n c u r v e [ b r ] − s h o u l d c r o s s w i t h f ( x ) a t y = x \mathrm{- \ swap \ y \ and \ x \ and \ rearrange \ etc}[br]f^{-1}(x) = \ln {( \sqrt {x + 1} + 2)} \,\, [3][br]domain: \, x \geq -1 \,\, [1][br]range: \, f^{-1}(x) \geq \ln 2 \,\, [1][br]\mathrm{- graph is reflection in y = x [2]}[br]\mathrm{- starts at (-1, ln 2) intercept at ln3, then curve}[br]\mathrm{- should cross with f(x) at y = x} − swap y and x and rearrange etc [ b r ] f − 1 ( x ) = ln ( x + 1 + 2 ) [ 3 ] [ b r ] d o main : x ≥ − 1 [ 1 ] [ b r ] r an g e : f − 1 ( x ) ≥ ln 2 [ 1 ] [ b r ] − graphisreflectioniny = x [ 2 ] [ b r ] − startsat ( − 1 , ln2 ) interceptatln3 , thencurve [ b r ] − shouldcrosswithf ( x ) aty = x Anything I missed or got wrong just ask. If you think it would be marked differently then say so too.