Section I Multiple choice
Complex numbers Polynomials
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Real coefficients make 3 − i 3-i 3 − i another root. The roots sum to 10, so the remaining root is 10 − ( 3 + i ) − ( 3 − i ) = 4 10-(3+i)-(3-i)=4 10 − ( 3 + i ) − ( 3 − i ) = 4 . Answer A:
a = 3 − i , b = 4 a=3-i,\ b=4 a = 3 − i , b = 4 .
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The length is ( − 2 ) 2 + 3 2 + ( − 6 ) 2 = 49 \sqrt{(-2)^2+3^2+(-6)^2}=\sqrt{49} ( − 2 ) 2 + 3 2 + ( − 6 ) 2 = 49 .
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The centre-radius equation is ( x + 1 ) 2 + ( y − 3 ) 2 + z 2 = 81 (x+1)^2+(y-3)^2+z^2=81 ( x + 1 ) 2 + ( y − 3 ) 2 + z 2 = 81 . Expanding gives x 2 + 2 x + y 2 − 6 y + z 2 = 71 x^2+2x+y^2-6y+z^2=71 x 2 + 2 x + y 2 − 6 y + z 2 = 71 .
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Complex numbers
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The modulus inequality is the closed disc centred at ( 2 , 3 ) (2,3) ( 2 , 3 ) with radius 1. The second condition is y ≤ x y\le x y ≤ x , so retain the small cap below the line y = x y=x y = x , including its boundary.
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Complex numbers
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The angle difference is the argument of 3 + 4 i 3+4i 3 + 4 i , modulo 2 π 2\pi 2 π . Its modulus is 5, so its sine is imaginary part divided by modulus. Answer B:
sin θ = 4 5 \sin\theta=\frac45 sin θ = 5 4 .
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Proof
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Change “for every” to “there exists”, change “there exists” to “for every”, and negate the equality. Keep the stated domains of the variables. Answer C:
∃ p > 0 such that ∀ q > p , q 2 ≠ p \exists p>0\text{ such that }\forall q>p,\ q^2\ne p ∃ p > 0 such that ∀ q > p , q 2 = p .
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Integration
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The decomposition is 1 7 ( x + 1 ) − 1 7 ( x − 6 ) + 1 ( x − 6 ) 2 \frac1{7(x+1)}-\frac1{7(x-6)}+\frac1{(x-6)^2} 7 ( x + 1 ) 1 − 7 ( x − 6 ) 1 + ( x − 6 ) 2 1 . Its primitive contains two logarithms and a term proportional to ( x − 6 ) − 1 (x-6)^{-1} ( x − 6 ) − 1 . Answer C; a primitive is
1 7 ln ∣ x + 1 ∣ − 1 7 ln ∣ x − 6 ∣ − 1 x − 6 + K \frac17\ln|x+1|-\frac17\ln|x-6|-\frac1{x-6}+K 7 1 ln ∣ x + 1∣ − 7 1 ln ∣ x − 6∣ − x − 6 1 + K .
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Complex numbers
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At the vertex 2 z − i z 2z-iz 2 z − i z , the two side vectors are i z iz i z and − 2 z -2z − 2 z . They are perpendicular, with lengths ∣ z ∣ |z| ∣ z ∣ and 2 ∣ z ∣ 2|z| 2∣ z ∣ , so the area is half their product.
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Vectors
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The second direction vector is − 2 -2 − 2 times the first. Also ( 3 , 2 , − 2 ) = ( 2 , 3 , − 4 ) + ( 1 , − 1 , 2 ) (3,2,-2)=(2,3,-4)+(1,-1,2) ( 3 , 2 , − 2 ) = ( 2 , 3 , − 4 ) + ( 1 , − 1 , 2 ) , so the second base point lies on the first line. The lines coincide, hence intersect and are parallel.
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Proof Calculus
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For option C, f ′ ′ ( x ) = 20 x 3 + 12 x 2 = 4 x 2 ( 5 x + 3 ) f^{\prime\prime}(x)=20x^3+12x^2=4x^2(5x+3) f ′′ ( x ) = 20 x 3 + 12 x 2 = 4 x 2 ( 5 x + 3 ) . This is zero at 0 but positive on both sides sufficiently close to 0, so concavity does not change there. Answer C:
f ( x ) = x 5 + x 4 f(x)=x^5+x^4 f ( x ) = x 5 + x 4 .
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Section II Written responses
Proof
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The contrapositive of “if P then Q” is “if not Q then not P”. For integers, not even means odd. Answer If a is odd, then a cubed is odd.
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Complex numbers
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Collect real and imaginary parts: 3 ( 3 + 2 i ) + ( − 1 − 5 i ) = 9 − 1 + ( 6 − 5 ) i 3(3+2i)+(-1-5i)=9-1+(6-5)i 3 ( 3 + 2 i ) + ( − 1 − 5 i ) = 9 − 1 + ( 6 − 5 ) i .
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Complex numbers
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Use z ˉ = 3 − 2 i \bar z=3-2i z ˉ = 3 − 2 i : 2 z ˉ w = 2 ( 3 − 2 i ) ( − 1 − 5 i ) = 2 ( − 13 − 13 i ) 2\bar zw=2(3-2i)(-1-5i)=2(-13-13i) 2 z ˉ w = 2 ( 3 − 2 i ) ( − 1 − 5 i ) = 2 ( − 13 − 13 i ) .
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Vectors
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Both position vectors have length 1. Their dot product gives cos θ = 1 / 10 \cos\theta=1/\sqrt{10} cos θ = 1/ 10 . Hence tan 2 θ = ( 1 − cos 2 θ ) / cos 2 θ \tan^2\theta=(1-\cos^2\theta)/\cos^2\theta tan 2 θ = ( 1 − cos 2 θ ) / cos 2 θ . Answer tan 2 θ = 9 \tan^2\theta=9 tan 2 θ = 9 .
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Complex numbers
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Put ( x + i y ) 2 = 11 + 60 i (x+iy)^2=11+60i ( x + i y ) 2 = 11 + 60 i . Then x 2 − y 2 = 11 x^2-y^2=11 x 2 − y 2 = 11 , x y = 30 xy=30 x y = 30 , and x 2 + y 2 = ∣ 11 + 60 i ∣ = 61 x^2+y^2=|11+60i|=61 x 2 + y 2 = ∣11 + 60 i ∣ = 61 . Thus x 2 = 36 x^2=36 x 2 = 36 , y 2 = 25 y^2=25 y 2 = 25 ; the signs agree because x y > 0 xy>0 x y > 0 . Answer 6 + 5 i 6+5i 6 + 5 i and
− 6 − 5 i -6-5i − 6 − 5 i .
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Complex numbers Proof
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If z = r e i θ z=re^{i\theta} z = r e i θ , then z ˉ = r e − i θ \bar z=re^{-i\theta} z ˉ = r e − i θ and ∣ z ∣ = r |z|=r ∣ z ∣ = r . Multiplying gives z z ˉ = r 2 e i θ − i θ = r 2 z\bar z=r^2e^{i\theta-i\theta}=r^2 z z ˉ = r 2 e i θ − i θ = r 2 . Answer z z ˉ = ∣ z ∣ 2 z\bar z=|z|^2 z z ˉ = ∣ z ∣ 2 .
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Integration
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Write 6 x − x 2 = 9 − ( x − 3 ) 2 6x-x^2=9-(x-3)^2 6 x − x 2 = 9 − ( x − 3 ) 2 . A primitive is sin − 1 ( ( x − 3 ) / 3 ) \sin^{-1}((x-3)/3) sin − 1 (( x − 3 ) /3 ) . At the limits x = 3 x=3 x = 3 and x = 3 / 2 x=3/2 x = 3/2 , the inverse sine values are 0 and − π / 6 -\pi/6 − π /6 .
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Complex numbers
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∣ z ∣ = a 2 |z|=a\sqrt2 ∣ z ∣ = a 2 since a > 0 a>0 a > 0 . The modulus of the fifth power is the fifth power of the modulus.Answer ∣ z 5 ∣ = 4 2 a 5 |z^5|=4\sqrt2\,a^5 ∣ z 5 ∣ = 4 2 a 5 .
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Complex numbers
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arg z = π / 4 \arg z=\pi/4 arg z = π /4 , so an argument of z 5 z^5 z 5 is 5 π / 4 5\pi/4 5 π /4 . Subtract 2 π 2\pi 2 π to enter the principal range ( − π , π ] (-\pi,\pi] ( − π , π ] .Answer Arg ( z 5 ) = − 3 π 4 \operatorname{Arg}(z^5)=-\frac{3\pi}4 Arg ( z 5 ) = − 4 3 π .
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Complex numbers Proof
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Expand the fourth power. Since ( 2 i ) 4 = 16 (2i)^4=16 ( 2 i ) 4 = 16 , the left side is 1 16 ( e 4 i θ − 4 e 2 i θ + 6 − 4 e − 2 i θ + e − 4 i θ ) \frac1{16}(e^{4i\theta}-4e^{2i\theta}+6-4e^{-2i\theta}+e^{-4i\theta}) 16 1 ( e 4 i θ − 4 e 2 i θ + 6 − 4 e − 2 i θ + e − 4 i θ ) . Pair conjugate exponentials using the supplied identity: e 4 i θ + e − 4 i θ = 2 cos 4 θ e^{4i\theta}+e^{-4i\theta}=2\cos4\theta e 4 i θ + e − 4 i θ = 2 cos 4 θ and e 2 i θ + e − 2 i θ = 2 cos 2 θ e^{2i\theta}+e^{-2i\theta}=2\cos2\theta e 2 i θ + e − 2 i θ = 2 cos 2 θ . Answer ( e i θ − e − i θ 2 i ) 4 = 1 8 ( cos 4 θ − 4 cos 2 θ + 3 ) \left(\frac{e^{i\theta}-e^{-i\theta}}{2i}\right)^4=\frac18(\cos4\theta-4\cos2\theta+3) ( 2 i e i θ − e − i θ ) 4 = 8 1 ( cos 4 θ − 4 cos 2 θ + 3 ) .
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Integration Trigonometry
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Euler’s sine identity identifies the fourth power in part (i) as sin 4 θ \sin^4\theta sin 4 θ . Integrate the three terms separately, dividing by each inner frequency. Answer ∫ sin 4 θ d θ = 3 θ 8 − sin 2 θ 4 + sin 4 θ 32 + C \int\sin^4\theta\,d\theta=\frac{3\theta}8-\frac{\sin2\theta}4+\frac{\sin4\theta}{32}+C ∫ sin 4 θ d θ = 8 3 θ − 4 s i n 2 θ + 32 s i n 4 θ + C .
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Polynomials Complex numbers
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Include the conjugate zeroes 1 − 6 i 1-6i 1 − 6 i and 3 + 4 i 3+4i 3 + 4 i . The conjugate pairs give ( x − 1 ) 2 + 36 (x-1)^2+36 ( x − 1 ) 2 + 36 and ( x − 3 ) 2 + 16 (x-3)^2+16 ( x − 3 ) 2 + 16 . Answer One example is
P ( x ) = ( x − 2 ) ( x 2 − 2 x + 37 ) ( x 2 − 6 x + 25 ) P(x)=(x-2)(x^2-2x+37)(x^2-6x+25) P ( x ) = ( x − 2 ) ( x 2 − 2 x + 37 ) ( x 2 − 6 x + 25 ) .
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Proof Inequalities
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Apply the given inequality to each factor: a + 7 b ≥ 2 7 a b a+7b\ge2\sqrt{7ab} a + 7 b ≥ 2 7 ab , b + 2 c ≥ 2 2 b c b+2c\ge2\sqrt{2bc} b + 2 c ≥ 2 2 b c , and c + 14 a ≥ 2 14 a c c+14a\ge2\sqrt{14ac} c + 14 a ≥ 2 14 a c . All factors are positive, so multiplication preserves the inequalities. Their product is at least 8 196 a 2 b 2 c 2 = 112 a b c 8\sqrt{196a^2b^2c^2}=112abc 8 196 a 2 b 2 c 2 = 112 ab c . Answer ( a + 7 b ) ( b + 2 c ) ( c + 14 a ) ≥ 112 a b c (a+7b)(b+2c)(c+14a)\ge112abc ( a + 7 b ) ( b + 2 c ) ( c + 14 a ) ≥ 112 ab c .
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Mechanics Simple harmonic motion
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The graph has period 4 and acceleration amplitude π 2 \pi^2 π 2 , starting at its maximum. Thus x ¨ = π 2 cos ( π t / 2 ) \ddot x=\pi^2\cos(\pi t/2) x ¨ = π 2 cos ( π t /2 ) . Integrating gives x ˙ = 2 π sin ( π t / 2 ) + C 1 \dot x=2\pi\sin(\pi t/2)+C_1 x ˙ = 2 π sin ( π t /2 ) + C 1 . Initial rest gives C 1 = 0 C_1=0 C 1 = 0 ; integrating again gives x = − 4 cos ( π t / 2 ) + C 2 x=-4\cos(\pi t/2)+C_2 x = − 4 cos ( π t /2 ) + C 2 . Use x ( 0 ) = − 2 x(0)=-2 x ( 0 ) = − 2 to obtain C 2 = 2 C_2=2 C 2 = 2 . Answer x ( t ) = 2 − 4 cos ( π t 2 ) x(t)=2-4\cos\left(\frac{\pi t}{2}\right) x ( t ) = 2 − 4 cos ( 2 π t ) .
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Integration
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Put u = e x u=e^x u = e x , so d u = e x d x du=e^x\,dx d u = e x d x . The integral becomes ∫ ( 1 + u ) / ( 1 + u 2 ) d u \int(1+u)/(1+u^2)\,du ∫ ( 1 + u ) / ( 1 + u 2 ) d u . Split it into ∫ d u / ( 1 + u 2 ) + ∫ u d u / ( 1 + u 2 ) \int du/(1+u^2)+\int u\,du/(1+u^2) ∫ d u / ( 1 + u 2 ) + ∫ u d u / ( 1 + u 2 ) , then substitute back. Answer tan − 1 ( e x ) + 1 2 ln ( 1 + e 2 x ) + C \tan^{-1}(e^x)+\frac12\ln(1+e^{2x})+C tan − 1 ( e x ) + 2 1 ln ( 1 + e 2 x ) + C .
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Proof
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Every positive multiple of 4 is 4 n 4n 4 n for a positive integer n n n . The displayed pattern suggests consecutive terms differing by 2: ( n + 1 ) 2 − ( n − 1 ) 2 = 4 n (n+1)^2-(n-1)^2=4n ( n + 1 ) 2 − ( n − 1 ) 2 = 4 n . Both bases are non-negative integers, so this supplies a difference of integer squares for every such multiple. Answer 4 n = ( n + 1 ) 2 − ( n − 1 ) 2 4n=(n+1)^2-(n-1)^2 4 n = ( n + 1 ) 2 − ( n − 1 ) 2 , for every integer
n ≥ 1 n\ge1 n ≥ 1 .
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Simple harmonic motion Mechanics
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Complete the square: v 2 = 16 − 2 ( x − 2 ) 2 v^2=16-2(x-2)^2 v 2 = 16 − 2 ( x − 2 ) 2 . The turning points occur at v = 0 v=0 v = 0 , giving x = 2 ± 2 2 x=2\pm2\sqrt2 x = 2 ± 2 2 , so the amplitude is 2 2 2\sqrt2 2 2 . One full period traverses four amplitudes, regardless of the starting point. Answer 8 2 m 8\sqrt2\text{ m} 8 2 m .
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Integration Trigonometry
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Let u = tan ( θ / 2 ) u=\tan(\theta/2) u = tan ( θ /2 ) . Then cos θ = ( 1 − u 2 ) / ( 1 + u 2 ) \cos\theta=(1-u^2)/(1+u^2) cos θ = ( 1 − u 2 ) / ( 1 + u 2 ) , sin θ = 2 u / ( 1 + u 2 ) \sin\theta=2u/(1+u^2) sin θ = 2 u / ( 1 + u 2 ) , and d θ = 2 d u / ( 1 + u 2 ) d\theta=2\,du/(1+u^2) d θ = 2 d u / ( 1 + u 2 ) . The integral simplifies to ∫ d u / ( u 2 − 2 u + 4 ) = ∫ d u / ( ( u − 1 ) 2 + 3 ) \int du/(u^2-2u+4)=\int du/((u-1)^2+3) ∫ d u / ( u 2 − 2 u + 4 ) = ∫ d u / (( u − 1 ) 2 + 3 ) . Answer 1 3 tan − 1 ( tan ( θ / 2 ) − 1 3 ) + C \frac1{\sqrt3}\tan^{-1}\left(\frac{\tan(\theta/2)-1}{\sqrt3}\right)+C 3 1 tan − 1 ( 3 t a n ( θ /2 ) − 1 ) + C , on each interval where the substitution is continuous.
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Mechanics Differential equations
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During descent, measure distance s s s downwards from the highest point and speed v ≥ 0 v\ge0 v ≥ 0 . Newton’s law gives v d v / d s = 10 − 0.1 v 2 v\,dv/ds=10-0.1v^2 v d v / d s = 10 − 0.1 v 2 . Let y = v 2 y=v^2 y = v 2 . Then d y / d s + 0.2 y = 20 dy/ds+0.2y=20 d y / d s + 0.2 y = 20 , with y ( 0 ) = 0 y(0)=0 y ( 0 ) = 0 , so v 2 = 100 ( 1 − e − s / 5 ) v^2=100(1-e^{-s/5}) v 2 = 100 ( 1 − e − s /5 ) . At the ground, s = 5 ln ( 676 / 100 ) s=5\ln(676/100) s = 5 ln ( 676/100 ) , hence v 2 = 100 ( 1 − 100 / 676 ) = 14400 / 169 v^2=100(1-100/676)=14400/169 v 2 = 100 ( 1 − 100/676 ) = 14400/169 . Answer v = 120 13 ≈ 9.23 m s − 1 v=\frac{120}{13}\approx9.23\text{ m s}^{-1} v = 13 120 ≈ 9.23 m s − 1 .
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Proof
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Suppose 6 = p / q \sqrt6=p/q 6 = p / q in lowest positive integer terms. Then p 2 = 6 q 2 p^2=6q^2 p 2 = 6 q 2 , so p p p is even; write p = 2 r p=2r p = 2 r . Then 2 r 2 = 3 q 2 2r^2=3q^2 2 r 2 = 3 q 2 , which makes q q q even too. This contradicts p p p and q q q having no common factor.
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Proof
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Suppose r = 3 − 2 r=\sqrt3-\sqrt2 r = 3 − 2 is rational. Squaring gives r 2 = 5 − 2 6 r^2=5-2\sqrt6 r 2 = 5 − 2 6 , hence 6 = ( 5 − r 2 ) / 2 \sqrt6=(5-r^2)/2 6 = ( 5 − r 2 ) /2 would be rational. This contradicts part (i). Answer 3 − 2 \sqrt3-\sqrt2 3 − 2 is irrational.
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Vectors Mechanics
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The squared distance to the transmitter is ( 3 − t / 4 ) 2 + 2 2 + ( t / 4 ) 2 (3-t/4)^2+2^2+(t/4)^2 ( 3 − t /4 ) 2 + 2 2 + ( t /4 ) 2 . Setting it to 9 gives t 2 − 12 t + 32 = 0 t^2-12t+32=0 t 2 − 12 t + 32 = 0 , so the helicopter first enters the 3 m boundary at t = 4 t=4 t = 4 s. At that instant its height is 52 m and its upward velocity is 1 / 4 m s − 1 1/4\text{ m s}^{-1} 1/4 m s − 1 . If τ \tau τ is time after power loss, height is 52 + τ / 4 − 5 τ 2 52+\tau/4-5\tau^2 52 + τ /4 − 5 τ 2 . Setting the height to zero gives 20 τ 2 − τ − 208 = 0 20\tau^2-\tau-208=0 20 τ 2 − τ − 208 = 0 . The positive root is ( 1 + 129 ) / 40 (1+129)/40 ( 1 + 129 ) /40 . Answer τ = 13 4 = 3.25 s \tau=\frac{13}{4}=3.25\text{ s} τ = 4 13 = 3.25 s .
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Integration Volumes
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Squaring y = x e x y=x\sqrt{e^x} y = x e x gives y 2 = x 2 e x y^2=x^2e^x y 2 = x 2 e x . The disc method gives V = π ∫ 0 3 x 2 e x d x V=\pi\int_0^3x^2e^x\,dx V = π ∫ 0 3 x 2 e x d x . Integrating by parts twice gives the primitive e x ( x 2 − 2 x + 2 ) e^x(x^2-2x+2) e x ( x 2 − 2 x + 2 ) . Evaluating at 3 and 0 yields 5 e 3 − 2 5e^3-2 5 e 3 − 2 . Answer V = π ( 5 e 3 − 2 ) V=\pi(5e^3-2) V = π ( 5 e 3 − 2 ) cubic units.
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Vectors
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With direction vector d = ( 6 , 2 , − 3 ) \mathbf d=(6,2,-3) d = ( 6 , 2 , − 3 ) , use B A → ⋅ d = 0 \overrightarrow{BA}\cdot\mathbf d=0 B A ⋅ d = 0 : ( 4 − 3 b , 5 − 4 b , 2 − 4 b ) ⋅ ( 6 , 2 , − 3 ) = 28 − 14 b = 0 (4-3b,5-4b,2-4b)\cdot(6,2,-3)=28-14b=0 ( 4 − 3 b , 5 − 4 b , 2 − 4 b ) ⋅ ( 6 , 2 , − 3 ) = 28 − 14 b = 0 .
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Vectors
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Now B = ( 6 , 8 , 8 ) B=(6,8,8) B = ( 6 , 8 , 8 ) , so ∣ A B ∣ = 4 + 9 + 36 = 7 |AB|=\sqrt{4+9+36}=7 ∣ A B ∣ = 4 + 9 + 36 = 7 . Triangle ABC is right-angled at A. With angle C equal to π / 4 \pi/4 π /4 , it has ∣ A C ∣ = ∣ A B ∣ = 7 |AC|=|AB|=7 ∣ A C ∣ = ∣ A B ∣ = 7 . The line direction ( 6 , 2 , − 3 ) (6,2,-3) ( 6 , 2 , − 3 ) also has length 7. Thus the two choices are C = A ± ( 6 , 2 , − 3 ) C=A\pm(6,2,-3) C = A ± ( 6 , 2 , − 3 ) . Answer O C → = ( 10 , 7 , − 1 ) \overrightarrow{OC}=(10,7,-1) OC = ( 10 , 7 , − 1 ) or
( − 2 , 3 , 5 ) (-2,3,5) ( − 2 , 3 , 5 ) .
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Mechanics Differential equations
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The equation of motion used here is d v / d t = − ( k + v 2 ) dv/dt=-(k+v^2) d v / d t = − ( k + v 2 ) . Separating and integrating from initial velocity u to velocity v gives t = − ∫ u v d s / ( k + s 2 ) t=-\int_u^v ds/(k+s^2) t = − ∫ u v d s / ( k + s 2 ) . Use ∫ d s / ( k + s 2 ) = k − 1 / 2 tan − 1 ( s / k ) \int ds/(k+s^2)=k^{-1/2}\tan^{-1}(s/\sqrt k) ∫ d s / ( k + s 2 ) = k − 1/2 tan − 1 ( s / k ) , since k > 0 k>0 k > 0 . Answer t = 1 k [ tan − 1 ( u k ) − tan − 1 ( v k ) ] t=\frac1{\sqrt k}\left[\tan^{-1}\left(\frac u{\sqrt k}\right)-\tan^{-1}\left(\frac v{\sqrt k}\right)\right] t = k 1 [ tan − 1 ( k u ) − tan − 1 ( k v ) ] .
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Mechanics Inequalities
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Substitute the given time in part (i): tan − 1 ( v / k ) = tan − 1 ( u / k ) − π / 4 \tan^{-1}(v/\sqrt k)=\tan^{-1}(u/\sqrt k)-\pi/4 tan − 1 ( v / k ) = tan − 1 ( u / k ) − π /4 . Since u > 0 u>0 u > 0 , the right side lies between − π / 4 -\pi/4 − π /4 and π / 4 \pi/4 π /4 . Therefore v < 0 v<0 v < 0 exactly when tan − 1 ( u / k ) < π / 4 \tan^{-1}(u/\sqrt k)<\pi/4 tan − 1 ( u / k ) < π /4 . Monotonicity of inverse tangent gives u < k u<\sqrt k u < k . Answer 0 < u < k 0<u<\sqrt k 0 < u < k , using the relation in part (i), with force in the fixed negative direction.
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Proof Induction
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Let S n = ∑ r = n + 1 2 n 1 / r S_n=\sum_{r=n+1}^{2n}1/r S n = ∑ r = n + 1 2 n 1/ r . For n = 2 n=2 n = 2 , S 2 = 1 / 3 + 1 / 4 = 14 / 24 > 13 / 24 S_2=1/3+1/4=14/24>13/24 S 2 = 1/3 + 1/4 = 14/24 > 13/24 . Assume S k > 13 / 24 S_k>13/24 S k > 13/24 for an integer k ≥ 2 k\ge2 k ≥ 2 . Comparing consecutive sums, S k + 1 − S k = 1 2 k + 1 + 1 2 k + 2 − 1 k + 1 = 1 ( 2 k + 1 ) ( 2 k + 2 ) > 0 S_{k+1}-S_k=\frac1{2k+1}+\frac1{2k+2}-\frac1{k+1}=\frac1{(2k+1)(2k+2)}>0 S k + 1 − S k = 2 k + 1 1 + 2 k + 2 1 − k + 1 1 = ( 2 k + 1 ) ( 2 k + 2 ) 1 > 0 . Thus S k + 1 > S k > 13 / 24 S_{k+1}>S_k>13/24 S k + 1 > S k > 13/24 , completing the induction. Answer ∑ r = n + 1 2 n 1 r > 13 24 \displaystyle\sum_{r=n+1}^{2n}\frac1r>\frac{13}{24} r = n + 1 ∑ 2 n r 1 > 24 13 for all integers
n > 1 n>1 n > 1 .
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Vectors
Show solution Hide solution for Question 15(b) +
The diagram shows P M PM PM perpendicular to the line. Write M = A + λ ( B − A ) = ( 1 + λ , − 1 + λ , 2 + λ ) M=A+\lambda(B-A)=(1+\lambda,-1+\lambda,2+\lambda) M = A + λ ( B − A ) = ( 1 + λ , − 1 + λ , 2 + λ ) , using direction ( 1 , 1 , 1 ) (1,1,1) ( 1 , 1 , 1 ) . Perpendicularity gives ( P − M ) ⋅ ( 1 , 1 , 1 ) = 0 (P-M)\cdot(1,1,1)=0 ( P − M ) ⋅ ( 1 , 1 , 1 ) = 0 , so ( 3 − λ ) − λ + ( 3 − λ ) = 0 (3-\lambda)-\lambda+(3-\lambda)=0 ( 3 − λ ) − λ + ( 3 − λ ) = 0 . Hence λ = 2 \lambda=2 λ = 2 and M = ( 3 , 1 , 4 ) M=(3,1,4) M = ( 3 , 1 , 4 ) . Because M is the midpoint, Q = 2 M − P Q=2M-P Q = 2 M − P . Answer Q = ( 2 , 3 , 3 ) Q=(2,3,3) Q = ( 2 , 3 , 3 ) .
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Complex numbers Sequences & series
Show solution Hide solution for Question 15(c) +
The first step runs from z 1 = 8 z_1=8 z 1 = 8 to z 2 = 6 i z_2=6i z 2 = 6 i , so its length is 8 2 + 6 2 = 10 \sqrt{8^2+6^2}=10 8 2 + 6 2 = 10 . Each subsequent difference is multiplied by 3 i / 4 3i/4 3 i /4 , so its length is multiplied by 3 / 4 3/4 3/4 . The total is the convergent geometric sum 10 / ( 1 − 3 / 4 ) 10/(1-3/4) 10/ ( 1 − 3/4 ) .
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Complex numbers
Show solution Hide solution for Question 15(d)(i) +
The radius is 1, so z 1 − w = cos ( − 2 π / 3 ) + i sin ( − 2 π / 3 ) = − 1 / 2 − i 3 / 2 z_1-w=\cos(-2\pi/3)+i\sin(-2\pi/3)=-1/2-i\sqrt3/2 z 1 − w = cos ( − 2 π /3 ) + i sin ( − 2 π /3 ) = − 1/2 − i 3 /2 . Add w = 2 + i w=2+i w = 2 + i . Answer z 1 = 3 2 + i ( 1 − 3 2 ) z_1=\frac32+i\left(1-\frac{\sqrt3}{2}\right) z 1 = 2 3 + i ( 1 − 2 3 ) .
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Complex numbers Vectors
Show solution Hide solution for Question 15(d)(ii) +
Write z 2 = x + i y z_2=x+iy z 2 = x + i y . The circle gives ( x − 2 ) 2 + ( y − 1 ) 2 = 1 (x-2)^2+(y-1)^2=1 ( x − 2 ) 2 + ( y − 1 ) 2 = 1 . A radius is perpendicular to its tangent, so ( x , y ) ⋅ ( x − 2 , y − 1 ) = 0 (x,y)\cdot(x-2,y-1)=0 ( x , y ) ⋅ ( x − 2 , y − 1 ) = 0 . Subtracting these equations gives 2 x + y = 4 2x+y=4 2 x + y = 4 . Substitution produces ( x − 2 ) ( 5 x − 6 ) = 0 (x-2)(5x-6)=0 ( x − 2 ) ( 5 x − 6 ) = 0 . The point shown above and to the left of the centre is ( 6 / 5 , 8 / 5 ) (6/5,8/5) ( 6/5 , 8/5 ) . Answer For the point shown,
z 2 = 6 5 + 8 5 i z_2=\frac65+\frac85i z 2 = 5 6 + 5 8 i . The other tangent point is
2 + 0 i 2+0i 2 + 0 i .
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Complex numbers Trigonometry
Show solution Hide solution for Question 16(a) +
Put z = e i θ z=e^{i\theta} z = e i θ , with 0 ≤ θ < 2 π 0\le\theta<2\pi 0 ≤ θ < 2 π . The imaginary-part condition becomes sin 3 θ + sin 2 θ + sin θ = 0 \sin3\theta+\sin2\theta+\sin\theta=0 sin 3 θ + sin 2 θ + sin θ = 0 . Using sin 3 θ + sin θ = 2 sin 2 θ cos θ \sin3\theta+\sin\theta=2\sin2\theta\cos\theta sin 3 θ + sin θ = 2 sin 2 θ cos θ , factor as sin 2 θ ( 2 cos θ + 1 ) = 0 \sin2\theta(2\cos\theta+1)=0 sin 2 θ ( 2 cos θ + 1 ) = 0 . The first factor gives θ = 0 , π / 2 , π , 3 π / 2 \theta=0,\pi/2,\pi,3\pi/2 θ = 0 , π /2 , π , 3 π /2 ; the second gives θ = 2 π / 3 , 4 π / 3 \theta=2\pi/3,4\pi/3 θ = 2 π /3 , 4 π /3 . Answer z ∈ { 1 , − 1 , i , − i , − 1 + i 3 2 , − 1 − i 3 2 } z\in\left\{1,-1,i,-i,\frac{-1+i\sqrt3}{2},\frac{-1-i\sqrt3}{2}\right\} z ∈ { 1 , − 1 , i , − i , 2 − 1 + i 3 , 2 − 1 − i 3 } .
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Integration Proof
Show solution Hide solution for Question 16(b)(i) +
Combine the integrands over the common denominator: 1 ( 1 + x 2 ) n − 1 ( 1 + x 2 ) n − 1 = 1 − ( 1 + x 2 ) ( 1 + x 2 ) n \frac1{(1+x^2)^n}-\frac1{(1+x^2)^{n-1}}=\frac{1-(1+x^2)}{(1+x^2)^n} ( 1 + x 2 ) n 1 − ( 1 + x 2 ) n − 1 1 = ( 1 + x 2 ) n 1 − ( 1 + x 2 ) . Integrating both sides from 0 to 1 gives the required relation. Answer I n − I n − 1 = ∫ 0 1 − x 2 ( 1 + x 2 ) n d x I_n-I_{n-1}=\displaystyle\int_0^1\frac{-x^2}{(1+x^2)^n}\,dx I n − I n − 1 = ∫ 0 1 ( 1 + x 2 ) n − x 2 d x .
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Integration
Show solution Hide solution for Question 16(b)(ii) +
First, I 1 = [ tan − 1 x ] 0 1 = π / 4 I_1=[\tan^{-1}x]_0^1=\pi/4 I 1 = [ tan − 1 x ] 0 1 = π /4 . To use part (i), differentiate x / ( 1 + x 2 ) x/(1+x^2) x / ( 1 + x 2 ) . Since d d x x 1 + x 2 = 1 − x 2 ( 1 + x 2 ) 2 \frac{d}{dx}\frac{x}{1+x^2}=\frac{1-x^2}{(1+x^2)^2} d x d 1 + x 2 x = ( 1 + x 2 ) 2 1 − x 2 , its integral is I 2 + ∫ 0 1 − x 2 ( 1 + x 2 ) 2 d x = I 2 + ( I 2 − I 1 ) I_2+\int_0^1\frac{-x^2}{(1+x^2)^2}\,dx=I_2+(I_2-I_1) I 2 + ∫ 0 1 ( 1 + x 2 ) 2 − x 2 d x = I 2 + ( I 2 − I 1 ) , using part (i). The boundary value is [ x / ( 1 + x 2 ) ] 0 1 = 1 / 2 [x/(1+x^2)]_0^1=1/2 [ x / ( 1 + x 2 ) ] 0 1 = 1/2 , so 2 I 2 − I 1 = 1 / 2 2I_2-I_1=1/2 2 I 2 − I 1 = 1/2 . Answer I 2 = 1 4 + π 8 I_2=\frac14+\frac\pi8 I 2 = 4 1 + 8 π .
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Vectors Proof
Show solution Hide solution for Question 16(c)(i) +
Expand the squared norm using the dot product: ∣ v ∣ 2 = cos 2 θ ∣ a ∣ 2 + sin 2 θ ∣ b ∣ 2 + 2 sin θ cos θ ( a ⋅ b ) |\mathbf v|^2=\cos^2\theta|\mathbf a|^2+\sin^2\theta|\mathbf b|^2+2\sin\theta\cos\theta(\mathbf a\cdot\mathbf b) ∣ v ∣ 2 = cos 2 θ ∣ a ∣ 2 + sin 2 θ ∣ b ∣ 2 + 2 sin θ cos θ ( a ⋅ b ) . A and B lie on the unit sphere, so their position vectors have length 1; they are perpendicular, so the cross term vanishes. Answer ∣ v ( θ ) ∣ 2 = cos 2 θ + sin 2 θ = 1 |\mathbf v(\theta)|^2=\cos^2\theta+\sin^2\theta=1 ∣ v ( θ ) ∣ 2 = cos 2 θ + sin 2 θ = 1 .
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Vectors
Show solution Hide solution for Question 16(c)(ii) +
Every point of C 1 C_1 C 1 satisfies y = 2 x y=2x y = 2 x , while every point of C 2 C_2 C 2 satisfies z = y z=y z = y . Thus an intersection has coordinates ( x , 2 x , 2 x ) (x,2x,2x) ( x , 2 x , 2 x ) . Both circles lie on the unit sphere, so x 2 + 4 x 2 + 4 x 2 = 1 x^2+4x^2+4x^2=1 x 2 + 4 x 2 + 4 x 2 = 1 , giving x = ± 1 / 3 x=\pm1/3 x = ± 1/3 . Each of these unit vectors lies in both circle planes. Answer ( 1 3 , 2 3 , 2 3 ) \left(\frac13,\frac23,\frac23\right) ( 3 1 , 3 2 , 3 2 ) and
( − 1 3 , − 2 3 , − 2 3 ) \left(-\frac13,-\frac23,-\frac23\right) ( − 3 1 , − 3 2 , − 3 2 ) .
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Vectors
Show solution Hide solution for Question 16(c)(iii) +
Take a = ( 0 , 1 , 0 ) \mathbf a=(0,1,0) a = ( 0 , 1 , 0 ) . The projection of O P → \overrightarrow{OP} OP onto this unit vector is ( 0 , 1 / 6 , 0 ) (0,1/\sqrt6,0) ( 0 , 1/ 6 , 0 ) . Subtract it to obtain r = ( 3 / 2 , 0 , − 1 / ( 2 3 ) ) \mathbf r=(\sqrt3/2,0,-1/(2\sqrt3)) r = ( 3 /2 , 0 , − 1/ ( 2 3 )) . This remainder has length 5 / 6 \sqrt{5/6} 5/6 . Normalising gives b = ( 3 / 10 , 0 , − 1 / 10 ) \mathbf b=(3/\sqrt{10},0,-1/\sqrt{10}) b = ( 3/ 10 , 0 , − 1/ 10 ) , perpendicular to a \mathbf a a . The vectors span the plane through O, A and P. Both are unit vectors, so the supplied circle formula applies; P occurs when cos θ = 1 / 6 \cos\theta=1/\sqrt6 cos θ = 1/ 6 and sin θ = 5 / 6 \sin\theta=\sqrt{5/6} sin θ = 5/6 . Answer v ( θ ) = cos θ ( 0 , 1 , 0 ) + sin θ 10 ( 3 , 0 , − 1 ) , 0 ≤ θ < 2 π \mathbf v(\theta)=\cos\theta\,(0,1,0)+\frac{\sin\theta}{\sqrt{10}}(3,0,-1),\quad0\le\theta<2\pi v ( θ ) = cos θ ( 0 , 1 , 0 ) + 10 s i n θ ( 3 , 0 , − 1 ) , 0 ≤ θ < 2 π .
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