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Page 1: GCE ‘A’ Level October/November 2010 Suggested Solutions ... · PDF fileMathematics H2 (9740/01 ) version 2.1 ... Paper 1 Suggested Solutions . ... GCE ‘A’ Level October/November

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Mathematics H2 (9740/01) version 2.1

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MATHEMATICS (H2) Paper 1 Suggested Solutions

9740/01 October/November 2010

1. Topic: Vectorsin Three Dimensions(Points & Lines)

(i) Given a = οΏ½2𝑝3𝑝6𝑝

οΏ½, b = οΏ½1

βˆ’22

οΏ½, where p > 0.

|𝐚| = p√22 + 32 + 62 = 7p

|𝐛| = οΏ½12 + (βˆ’2)2 + (2)2 = 3

Since|𝐚| = |𝐛| 7p = 3

∴ p = πŸ‘πŸ•

(ii) a = 37

οΏ½236

οΏ½ =

⎝

βŽœβŽ›

6797

187 ⎠

⎟⎞

(a +b)βˆ™(a – b) =

⎣⎒⎒⎒⎑

⎝

βŽœβŽ›

6797

187 ⎠

⎟⎞

+ οΏ½1

βˆ’22

οΏ½

⎦βŽ₯βŽ₯βŽ₯⎀

βˆ™

⎣⎒⎒⎒⎑

⎝

βŽœβŽ›

6797

187 ⎠

⎟⎞

βˆ’ οΏ½1

βˆ’22

οΏ½

⎦βŽ₯βŽ₯βŽ₯⎀

=

⎝

βŽœβŽ›

137

βˆ’57

327 ⎠

⎟⎞

βˆ™

⎝

βŽœβŽ›

βˆ’17

23747 ⎠

⎟⎞

= βˆ’1349

βˆ’ 11549

+ 12849

= 0

∴ (a +b) βˆ™(a – b) = 0 (shown)

ALTERNATIVE APPROACH

(a + b) βˆ™(a – b) = aβˆ™a –aβˆ™b + aβˆ™b–bβˆ™b = |𝐚|2 βˆ’ |𝐛|2 = |𝐚|2 βˆ’ |𝐚|2(since |𝐚| = |𝐛|) = 0

2. Topic: Maclaurin’s Series

(i) eπ‘₯(1 + sin 2π‘₯)

= οΏ½1 + π‘₯ + 12

π‘₯2 + β‹― οΏ½ [1 + 2π‘₯ βˆ’ β‹― ]

= 1 + 2π‘₯ + π‘₯ + 2π‘₯2 + 12

π‘₯2 + β‹―

= 𝟏 + πŸ‘π’™ + πŸ“πŸ

π’™πŸ + ⋯………….………………… (1)

(ii) (1 + 43

π‘₯)𝑛

= 1 + 𝑛1

(43

π‘₯)1 + 𝑛(π‘›βˆ’1)2!

(43

π‘₯)2 + β‹―

= 1 + 43

𝑛π‘₯ + 89

𝑛(𝑛 βˆ’ 1)π‘₯2 + β‹― ………………… (2)

Comparing coefficients of x in (1) and (2)

43

𝑛 = 3

𝒏 = πŸ—πŸ’

∴ Third term in series (2)

= πŸ–πŸ—

οΏ½πŸ—πŸ’οΏ½ οΏ½πŸ—

πŸ’βˆ’ 𝟏� π’™πŸ

= πŸ“πŸ

π’™πŸ

= Third term in series (1) (shown)

eπ‘₯ = 1 + π‘₯ +π‘₯2

2! +π‘₯3

3! + β‹― +π‘₯π‘Ÿ

π‘Ÿ! + β‹―

sin π‘₯ = π‘₯ βˆ’π‘₯3

3! +π‘₯5

5! βˆ’ β‹―(βˆ’1)π‘Ÿπ‘₯2π‘Ÿ+1

(2π‘Ÿ + 1)! + β‹―

From MF15:

𝐚 βˆ™ 𝐚 = |𝐚|2

From MF15: (1 + π‘₯)𝑛 = 1 + 𝑛π‘₯ + 𝑛(π‘›βˆ’1)

2!π‘₯2 + β‹―

Sub 2x into sin x expansion

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3. Topic: Arithmetic Progression, Recurrence (i) Given Sn = n(2n + c) un = Sn βˆ’ Snβˆ’1

= n (2n + c) – (n βˆ’ 1) [2(n – 1) + c]

= 2n2 + nc – 2(n – 1)2 – c (n – 1)

= 2n2 + nc – 2 (n2 – 2n + 1) – cn + c

= 4n + c – 2

ALTERNATIVE APPROACH

S1 = u1 = 1[2(1) + c] = 2 + c

S2 = u2 + u1 = 2[4 + c] = 8 + 2c

β‡’ u2 = S2 βˆ’ S1 = 8 + 2c βˆ’ 2 – c = 6 + c

S3 = u3 + u2 + u1 = 3(6 + c) = 18 + 3c

β‡’ u3 = S3 – S2 = 18 + 3c βˆ’ 8 βˆ’ 2c = 10 + c

S4 = u4 + u3 + u2 + u1 = 4[8 + 2c] = 32 + 4c

β‡’ u4 = S4 – S3 = 32 + 4c βˆ’ 18 βˆ’ 3c = 14 + c

Since u2 βˆ’ u1 = u3 βˆ’ u2 = u4 βˆ’ u3 = 4

β‡’ un is an arithmetic progression (A. P.).

∴un = 2 + c + (n – 1) 4

= 2 + c + 4n – 4

= 4n + c– 2

(ii) un = 4n + c – 2

un+1 = 4(n + 1) + c – 2

= 4n + 4 + c – 2

= (4n + c – 2) + 4

= un + 4

ALTERNATIVE APPROACH

From un in (i):

u1 = 2 + c

u2 = 6 + c = 4 + (2 + c) = 4 + u1

u3 = 10 + c = 4 + (6 + c) = 4 + u2

u4 = 14 + c = 4 + (10 + c) = 4 + u3

∴un+1 = 4 + un

1st term, a = 2 + c Common difference, d = 4

nth term in an A.P.: Tn = a + (n – 1) d

f(un) = 4 + un

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4. Topic: Differentiation (Tangents &Normals)

(i) Given x2 – y2 + 2xy + 4 = 0………………… (1)

Using implicit differentiation,

2π‘₯ βˆ’ 2𝑦 d𝑦dπ‘₯

+ οΏ½2𝑦 + 2π‘₯ d𝑦dπ‘₯

οΏ½ = 0

π‘₯ + 𝑦 = (𝑦 βˆ’ π‘₯) d𝑦dπ‘₯

βˆ΄ππ’šππ’™

= 𝒙+π’šπ’šβˆ’π’™

(ii) For the tangent of the curve to be parallel to the x-axis,

d𝑦dπ‘₯

= 0

β‡’ π‘₯+π‘¦π‘¦βˆ’π‘₯

= 0

y = βˆ’ x ……………… (2) Sub (2) into (1) x2 – (βˆ’ x)2 + 2x(βˆ’ x) + 4 = 0 x2 – x2 – 2x2 + 4 = 0 2x2 = 4

x = ±√2

Sub x = βˆ’ √2 into (2)

y = √2

Sub x= √2 into (2)

y = βˆ’ √2

The coordinates are (βˆ’βˆšπŸ, √𝟐) and (√𝟐, βˆ’βˆšπŸ).

5. Topic: Functions, Graphs (Transformations)

(i) Given y = x3 = f(x) y = (x – 2)3 = g(x)

y = 12(x – 2)3 = h(x)

y = 𝟏𝟐(x – 2)3βˆ’ 6

When x = 0, y = 12(βˆ’2)3 – 6

= βˆ’ 10

When y = 0, 0 = 12(x – 2)3 βˆ’ 6

(x – 2)3 = 12

x = 2 + √123

∴Curve crosses the y-axis at (0, βˆ’10) and the x-axis at (2 +βˆšπŸπŸπŸ‘ , 0).

f(x – 2) Translate 2 units in the positive x- direction

12g(x)

Stretch with scale factor 12 parallel to the y- axis

h(x)– 6 Translate 6 units in the negative y -direction

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(ii) Using G. C. (refer to Appendix for detailed steps),

For y = fβˆ’1(x), when y = 0, x = βˆ’10 x = 0, y = 2 + βˆšπŸπŸπŸ‘

6. Topic: Integration

(i) Using G.C. for y = x3 βˆ’ 3x + 1 (refer to Appendix for detailed steps and various methods that can be used),

β = 0.3473, γ = 1.5321 ∴β = 0.347 andγ= 1.532(3d.p.)

(ii) Using G.C. (refer to Appendix for detailed steps and various methods used),

Area ofthe region bounded by the curve and the x- axis (between x = 𝛽 and x = 𝛾) = �∫ (π‘₯3 βˆ’ 3π‘₯ + 1)𝛾

𝛽 dπ‘₯οΏ½ = | (βˆ’0.7814168)|

β‰ˆ 0.781 units2(3sig.fig.)

The graph of y = fβˆ’1(x) is obtained by reflecting the graph of y = f(x) in the line y = x.

Remember to obtain the absolute value for the answer as we are finding the area.

The x-coordinate in f(x) becomes the y-coordinate in fβˆ’1(x) and vice versa.

y = x y = f(x)

y = fβˆ’1(x)

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(iii) Obtain the x-coordinates of the intersection points for y = x3 – 3x + 1 ………………… (1) y = 1 ………………… (2) (1) = (2) x3– 3x + 1 = 1 x(x2 – 3) = 0

x = 0, x = ±√3

From the diagram, the lower and upper limit of integration to find the region is βˆ’βˆš3 and 0 respectively. Hence, area of region (shaded region A) between the curve and the line

= ∫ (π‘₯3 βˆ’ 3π‘₯ + 1)dπ‘₯0βˆ’βˆš3 βˆ’ οΏ½1 Γ— √3οΏ½

= οΏ½14

π‘₯4 βˆ’ 32

π‘₯2 + π‘₯οΏ½βˆ’βˆš3

0βˆ’ √3

= οΏ½0 βˆ’ οΏ½14

Γ— 9 βˆ’ 32

(3) βˆ’ √3οΏ½οΏ½ βˆ’ √3

= βˆ’ 94

+ 92

+ √3 βˆ’ √3

= πŸ—πŸ’ units2

(iv)

Sincex = βˆ’1 and x = 1 are stationary points, When x = βˆ’1, ymax = (βˆ’1)3 – 3(βˆ’1) + 1 = 3 When x = 1, ymin = (1)3 – 3(1) + 1 = βˆ’1 For x3 – 3x + 1 = k to have three real distinct roots,

ymin<k<ymax ∴Set of values of k = {kπ›œ ℝ: βˆ’1<k <3} Area of rectangle

Check final answer with G. C. (time permitting)

Note: β€’ Final answer expressed in set notation as

question asks for set of values of k. β€’ Three real distinct roots β‡’ no equal sign

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7. Topic: Differential Equations

Given dπœƒd𝑑

∝ (20 βˆ’ πœƒ)

β‡’dπœƒd𝑑

= π‘˜(20 βˆ’ πœƒ), where k is a constant………………… (1)

Whent = 0, sub ΞΈ = 10 and dπœƒd𝑑

= 1 into (1)

1 = k (20 – 10)

k = 120βˆ’10

= 110

β‡’dπœƒd𝑑

= 110

(20 βˆ’ πœƒ)

∫ 120βˆ’πœƒ

dπœƒ = ∫ 110

d𝑑

βˆ’ ln|20 βˆ’ πœƒ| = 110

𝑑 + 𝑐

When t = 0,ΞΈ = 10 βˆ’ ln|20 βˆ’ 10| = 0 + c c = βˆ’ ln 10

β‡’ βˆ’ ln|20 βˆ’ πœƒ| = 110

𝑑 βˆ’ ln 10

ln(20 βˆ’ πœƒ) = βˆ’ 110

+ ln 10

20 – ΞΈ = eβˆ’ 110𝑑 βˆ™ eln 10

20 – ΞΈ = 10eβˆ’ 110𝑑

∴θ = 𝟐𝟎 βˆ’ πŸπŸŽπžβˆ’ πŸπŸπŸŽπ’• (shown)…………………………… (2)

Sub ΞΈ = 15 into (2), 15 = 20 βˆ’ 10eβˆ’ 1

10𝑑

10eβˆ’ 110𝑑 = 5

eβˆ’ 110𝑑 = 1

2

t = βˆ’10 ln 12

= 10 π₯𝐧 𝟐 mins

From (2), ΞΈ = 20 βˆ’ 10eβˆ’ 110𝑑

As tβ†’βˆž, eβˆ’ 110𝑑 β†’ 0 β‡’ ΞΈ β†’ 20

∴θ approaches 20°C for large values oft.

Using G.C. (refer to Appendix for detailed steps),

t 0

20

ΞΈ

10

ΞΈ = 20 βˆ’ 10eβˆ’ 110𝑑

eln π‘₯ = π‘₯

οΏ½1π‘₯

dπ‘₯ = ln|π‘₯| + 𝑐

οΏ½ g(𝑦) d𝑦 = οΏ½ f(π‘₯) dπ‘₯

Variable separable form

t

ΞΈ

10

0

20 ΞΈ is always ≀ 20

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8. Topic: Complex Numbers (Polar Form, Loci & Argand Diagrams)

(i) z1 = 1 + i√3

|𝑧1| = οΏ½12 + �√3οΏ½2 = 2

ΞΈ1 = tanβˆ’1 �√31

οΏ½ = Ο€3

∴z1 = 𝟐 �𝐜𝐨𝐬 π…πŸ‘

+ 𝐒 𝐬𝐒𝐧 π…πŸ‘

οΏ½

z2 = βˆ’1 – i

|𝑧2| = οΏ½(βˆ’1)2 + (βˆ’1)2 = √2

ΞΈ2 = βˆ’Ο€ + tanβˆ’1 οΏ½βˆ’1βˆ’1

οΏ½ = βˆ’ 3Ο€4

∴z2 = √𝟐 �𝐜𝐨𝐬 οΏ½βˆ’ πŸ‘π›‘πŸ’

οΏ½ + 𝐒 𝐬𝐒𝐧 οΏ½βˆ’ πŸ‘π›‘πŸ’

οΏ½οΏ½

(ii) z1 = 2 οΏ½cos Ο€3

+ i sin Ο€3

οΏ½ = 2eiπœ‹3

z2 = √2(cos οΏ½βˆ’ 3Ο€4

οΏ½ + i sin οΏ½βˆ’ 3Ο€4

οΏ½ = √2eiοΏ½βˆ’3Ο€4 οΏ½

𝑧1𝑧2

= 2eiΟ€3

√2eiοΏ½βˆ’3Ο€4 οΏ½

= 2√2

eiοΏ½Ο€3βˆ’οΏ½βˆ’3Ο€

4 οΏ½οΏ½

= √2eiοΏ½1312Ο€οΏ½

= √2eiοΏ½βˆ’1112Ο€οΏ½

= √2 οΏ½cos οΏ½βˆ’ 1112

Ο€οΏ½ + i sin οΏ½βˆ’ 1112

Ο€οΏ½οΏ½

βˆ΄οΏ½π‘§1𝑧2

οΏ½βˆ— = √2 οΏ½cos οΏ½βˆ’ 11

12Ο€οΏ½ βˆ’ i sin οΏ½βˆ’ 11

12Ο€οΏ½οΏ½

= √𝟐 �𝐜𝐨𝐬 �𝟏𝟏𝟏𝟐

𝛑� + 𝐒 𝐬𝐒𝐧 �𝟏𝟏𝟏𝟐

𝛑��

ALTERNATIVE APPROACH

��𝑧1𝑧2

οΏ½βˆ—οΏ½ = �𝑧1

𝑧2οΏ½

= |𝑧1||𝑧2|

= 2√2

= √2

arg�𝑧1𝑧2

οΏ½βˆ— = βˆ’arg�𝑧1

𝑧2οΏ½

= βˆ’ οΏ½πœ‹3

βˆ’ οΏ½βˆ’ 3πœ‹4

οΏ½οΏ½

= βˆ’ 13πœ‹12

= 11πœ‹12

βˆ΄οΏ½π‘§1𝑧2

οΏ½βˆ— = √𝟐 �𝐜𝐨𝐬 �𝟏𝟏

πŸπŸπ›‘οΏ½ + 𝐒 𝐬𝐒𝐧 �𝟏𝟏

πŸπŸπ›‘οΏ½οΏ½

Complex conjugate z = a + ib z* = aβˆ’ib

Arg �𝑧1

𝑧2οΏ½ =

13Ο€12

βˆ’ 2Ο€ = βˆ’11Ο€12

Principal argument (βˆ’Ο€ < ΞΈ ≀ Ο€)

arg (z*) = βˆ’ arg (z)

|π‘§βˆ—| = |𝑧|

Arg �𝑧1

𝑧2οΏ½

βˆ—= βˆ’

13Ο€12

+ 2Ο€ =11Ο€12

Principal argument (βˆ’Ο€ < ΞΈ ≀ Ο€)

cos(βˆ’πœƒ)= cos πœƒ sin(βˆ’πœƒ)= βˆ’sin πœƒ

𝑧 = π‘₯ + i𝑦 = π‘Ÿ(cos πœƒ + i sin πœƒ) Polar Form:

where π‘Ÿ = |𝑧| = οΏ½π‘₯2 + 𝑦2 πœƒ = tanβˆ’1 𝑦

π‘₯

1

Im

Re βˆ’1

z2 βˆ’1 ΞΈ2

√3 z1

ΞΈ1

𝑧 = π‘Ÿ(cos πœƒ + i sin πœƒ) = π‘Ÿeiπœƒ Exponential Form:

arg�𝑧1𝑧2

οΏ½ = arg (z1) – arg (z2)

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(iii) (a) |𝑧 βˆ’ 𝑧1| = 2

�𝑧 βˆ’ (1 + i √3)οΏ½ = 2

(b) arg (z – z2) = πœ‹4

arg[z – (βˆ’1 – i)] = πœ‹4

(iv) CO = CA = 2 β‡’ βˆ† COA is isosceles. CMβŠ₯OA β‡’ OM = MA = 1. ∴OA = OM + MA = 1 +1 = 2.

∴The locus |𝒛 βˆ’ π’›πŸ| = 2 meets the positive real axis at (2, 0).

ALTERNATIVE APPROACH

Cartesian equation of |𝑧 βˆ’ 𝑧1| = 2 loci:

(x – 1)2 + (yβˆ’βˆš3)2 = 22

Sub y = 0, (x – 1)2 + 3 = 22 (x – 1)2 = 1 x – 1 = Β±1 x = 0 (reject), 2

∴The locus |𝒛 βˆ’ π’›πŸ| = 2 meets the positive real axis at (2, 0).

0

C

Im(z)

2

√3

Re(z) 1

1

βˆ’1

βˆ’1

|𝑧 βˆ’ 𝑧1| = 2 arg (z – z2) = πœ‹4

Ο€4

O

C

M Re(z)

Im(z)

A

2

2

1

√3

β‡’ circle with center C (1, √3) and radius 2 units.

β‡’straight line beginning at (βˆ’1, βˆ’1) with an angle of πœ‹

4 rad with respect

to the Re(z) axis.

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GCE β€˜A’ Level October/November 2010 Suggested Solutions

Mathematics H2 (9740/01) version 2.1

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9. Topic: Differentiation (Maxima & Minima)

(i) Volume of box = x(3x)y 300 = 3x2y

y = 100π‘₯2 cm …………………… (1)

External surface area of box, A1 = x(3x) + 2yx + 2y(3x) = (3x2 + 8xy) cm2

External surface area of lid, A2 = x(3x) + 2(ky)x + 2(ky)(3x) = (3x2 + 8kxy) cm2

Total external surface area of the box and the lid, A = A1 + A2 = (3x2 + 8xy) + (3x2 + 8kxy) = 6x2 + 8(1 + k) xy

= 6π‘₯2 + 8(1 + π‘˜)π‘₯ οΏ½100π‘₯2 οΏ½

A = 6π‘₯2 + 800(1 + π‘˜)π‘₯

d𝐴dπ‘₯

= 12π‘₯ βˆ’ 800(1 + π‘˜)π‘₯2 …………………… (2)

d2𝐴dπ‘₯2 = 12 + 1600(1 + π‘˜)

π‘₯3 …………………… (3)

Stationary point of A occurs when d𝐴dπ‘₯

= 0.

From (2), 12x – 800(1+π‘˜)π‘₯2 = 0

12x = 800(1+π‘˜)π‘₯2

x3 = 200(1+π‘˜)3

x = οΏ½200(1+π‘˜)3

οΏ½13

Using second derivative test, sub x = οΏ½200(1+π‘˜)3

οΏ½13into (3),

d2𝐴dπ‘₯2 = 12 + 1600(1+π‘˜)

οΏ½οΏ½200(1+π‘˜)3 οΏ½

13οΏ½

3

= 12 + 1600(1 + π‘˜) Γ— 3200(1+π‘˜)

= 36 >0

β‡’ Ais minimum when x = �𝟐𝟎𝟎(𝟏+π’Œ)πŸ‘

οΏ½πŸπŸ‘

(ii) From (1) y = 100π‘₯2

𝑦π‘₯ = 100

π‘₯3

= 100

οΏ½οΏ½200(1+π‘˜)3 οΏ½

13οΏ½

3

= 100 οΏ½ 3200(1+π‘˜)

οΏ½

= πŸ‘πŸ(𝟏+π’Œ)

(iii) Given 0 < k ≀ 1 1 < 1 + k ≀ 2 2 < 2(1 + k) ≀ 4

14 ≀ 1

2(1+π‘˜) < 1

2

34 ≀ 3

2(1+π‘˜) < 3

2

∴ πŸ‘πŸ’ ≀ π’š

𝒙 < πŸ‘

𝟐

Sub x = οΏ½200(1+π‘˜)3

οΏ½13

Manipulate k to get 3

2(1+π‘˜) = π’š

𝒙

Sub y = 100π‘₯2

Second Derivative Test:

Sign of ππŸπ’š

ππ’™πŸ Nature of stationary point

βˆ’ Maximum + Minimum 0 Point of inflexion

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Mathematics H2 (9740/01) version 2.1

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ALTERNATIVE APPROACH 𝑦π‘₯ = 3

2(1+π‘˜) β†’ Let Y = 𝑦

π‘₯ and X = k β‡’ Y = 3

2(1+X)

Using G.C. to obtain range of Y for 0 < X ≀ 1 (refer to Appendix for detailed steps),

Given 0 < k ≀ 1

∴ πŸ‘πŸ’ ≀ π’š

𝒙 < πŸ‘

𝟐

(iv) For the box to have square ends, y = x.

From (ii), 𝑦π‘₯ = 3

2(1+π‘˜)

1 = 32(1+π‘˜)

1 + k = 32

k = 𝟏𝟐

10.

Topic: Vectors in Three Dimensions (Lines &Planes)

(i) l: π‘₯βˆ’10βˆ’3

= 𝑦+16

= 𝑧+39

β‡’ r = οΏ½10βˆ’1βˆ’3

οΏ½ + πœ† οΏ½βˆ’369

οΏ½ , πœ† ∈ ℝ……………. (1)

r = οΏ½10βˆ’1βˆ’3

οΏ½ + πœ‡ οΏ½βˆ’123

οΏ½ , where πœ‡ = 3πœ†

β‡’ direction vector of l, d = οΏ½βˆ’123

οΏ½

p: x – 2y – 3z = 0

β‡’ 𝐫 βˆ™ οΏ½1

βˆ’2βˆ’3

οΏ½ = 0 ……………………………… (2)

β‡’ normal of plane p, n = οΏ½1

βˆ’2βˆ’3

οΏ½ = βˆ’οΏ½βˆ’123

οΏ½

Since n = βˆ’ d, l is parallel to normal, n.

∴l is perpendicular to plane p. (shown)

(ii) From (1), r = οΏ½10 βˆ’ πœ‡

βˆ’1 + 2πœ‡βˆ’3 + 3πœ‡

�……… (3)

At intersection point, sub (3) into (2),

οΏ½10 βˆ’ πœ‡

βˆ’1 + 2πœ‡βˆ’3 + 3πœ‡

οΏ½ βˆ™ οΏ½1

βˆ’2βˆ’3

οΏ½ = 0

10 – πœ‡ + 2 βˆ’ 4πœ‡ + 9 βˆ’ 9πœ‡ = 0 21βˆ’ 14πœ‡ = 0

πœ‡ = 32

π‘₯ βˆ’ π‘Ž1

𝑑1=

𝑦 βˆ’ π‘Ž2

𝑑2=

𝑧 βˆ’ π‘Ž3

𝑑3

r = οΏ½π‘Ž1π‘Ž2π‘Ž3

οΏ½ + πœ† �𝑑1𝑑2𝑑3

οΏ½ , Ξ» ∈ ℝ

Equation of Line:

Cartesian form

Vector form

𝑛1π‘₯ + 𝑛2𝑦 + 𝑛3𝑧 = 𝐷

r β‹… �𝑛1𝑛2𝑛3

� = 𝐷

Equation of Plane:

Cartesian form

Standard form

0 X 1

0.75

1.5

Y = 32(1+X)

Y

Inclusive (≀)

Exclusive (<)

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Mathematics H2 (9740/01) version 2.1

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Sub πœ‡ = 32 into (2),

r =

⎝

βŽœβŽ›

10 βˆ’ 32

βˆ’1 + 2 οΏ½32οΏ½

βˆ’3 + 3 οΏ½32�⎠

⎟⎞

= οΏ½

172232

οΏ½

∴ Coordinates of the point of intersection of l and p is (πŸπŸ•πŸ

, 𝟐, πŸ‘πŸ ).

(iii) Sub A (βˆ’2, 23, 33) into (1),

οΏ½βˆ’22333

οΏ½ = οΏ½10βˆ’1βˆ’3

οΏ½ + πœ‡ οΏ½βˆ’123

οΏ½

πœ‡ οΏ½βˆ’123

οΏ½ = οΏ½βˆ’122436

οΏ½

πœ‡ οΏ½βˆ’123

οΏ½ = 12 οΏ½βˆ’123

οΏ½

πœ‡ = 12

Since there is a valid solution forΒ΅, point A lies on l.

From (2), r βˆ™ οΏ½1

βˆ’2βˆ’3

οΏ½=0 β‡’ Origin O lies on plane p.

Using Midpoint Theorem,

𝑂𝑀������⃗ = 𝑂𝐴������⃗ +𝑂𝐡������⃗

2

𝑂𝐡�����⃗ = 2𝑂𝑀������⃗ βˆ’ 𝑂𝐴�����⃗

= 2οΏ½

172232

οΏ½ βˆ’ οΏ½βˆ’22333

οΏ½

= οΏ½19

βˆ’19βˆ’30

οΏ½

∴ Coordinates of the point B is (19, βˆ’19, βˆ’ 30).

M(172

, 2,32) O

A (βˆ’2, 23, 33)

p

B

l

Midpoint Theorem:

If M is the midpoint of AB, then 𝐦 = 𝐚+𝐛

2

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(iv) Area of βˆ†OAB = 12

�𝑂𝐴�����⃗ Γ— 𝑂𝐡�����⃗ οΏ½

= 12

οΏ½οΏ½βˆ’22333

οΏ½ Γ— οΏ½19

βˆ’19βˆ’30

οΏ½οΏ½

= 12

οΏ½οΏ½βˆ’63567

βˆ’399οΏ½οΏ½

= 12

οΏ½(βˆ’63)2 + (567)2 + (βˆ’399)2

= 348.087 β‰ˆ 348 unit2

11. Topic:Differentiation, Parametric Equations & Graphs

(i) Given x = t + 1𝑑 and y = t βˆ’ 1

𝑑

dπ‘₯d𝑑

= 1 βˆ’ 1𝑑2 d𝑦

d𝑑 = 1 + 1

𝑑2

= 𝑑2βˆ’1𝑑2 = 𝑑2+1

𝑑2

β‡’d𝑦dπ‘₯

= d𝑦d𝑑dπ‘₯d𝑑

= 𝑑2+1𝑑2βˆ’1

At point P,t = p,

x = 𝑝 + 1𝑝 and y = 𝑝 βˆ’ 1

𝑝

d𝑦dπ‘₯

= 𝑝2+1𝑝2βˆ’1

Equation of tangent at point P:

𝑦 βˆ’ �𝑝 βˆ’ 1𝑝

οΏ½ = 𝑝2+1𝑝2βˆ’1

οΏ½π‘₯ βˆ’ �𝑝 + 1𝑝

οΏ½οΏ½

𝑦 βˆ’ �𝑝2βˆ’1𝑝

οΏ½ = 𝑝2+1𝑝2βˆ’1

(π‘₯) βˆ’ �𝑝2+1𝑝2βˆ’1

οΏ½ �𝑝2+1𝑝

οΏ½

p(p2 – 1) y – (p2 – 1)(p2 – 1) = p (p2 + 1) x βˆ’ (p2 + 1)(p2 + 1)

p(p2 – 1) y – p4 + 2p2 – 1 = p (p2 + 1) x – p4 βˆ’ 2p2 – 1

p(p2 – 1) y = p (p2 + 1) x – 4p2

(p2 – 1)y = (p2 + 1) x – 4p (p2 + 1) x – (p2 – 1)y = 4p (shown)

Gradient of tangent at point (x1, y1) = π‘¦βˆ’π‘¦1

π‘₯βˆ’π‘₯1

οΏ½π‘Ž1π‘Ž2π‘Ž3

οΏ½ Γ— �𝑏1𝑏2𝑏3

οΏ½ = οΏ½π‘Ž2𝑏3 βˆ’ π‘Ž3𝑏2π‘Ž3𝑏1 βˆ’ π‘Ž1𝑏3π‘Ž1𝑏2 βˆ’ π‘Ž2𝑏1

οΏ½

Vector Product:

d𝑦d𝑑

=d𝑦dπ‘₯

Γ—dπ‘₯d𝑑

Chain Rule:

Gradient of tangent at point P.

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(ii)

Equation of tangent at P, (p2 + 1) x – (p2 – 1) y = 4p ……………………(1) At point A, sub y = x into (1) [(𝑝2 + 1) βˆ’ (𝑝2 βˆ’ 1)]π‘₯ = 4p x = 2p β‡’ y = 2p

β‡’A (2p, 2p)

At point B, sub y = βˆ’ x into (1)

[𝑝2 + 1 + 𝑝2 βˆ’ 1]π‘₯ = 4p 2p2x = 4p

x = 2𝑝 β‡’ y = βˆ’ 2

𝑝

⇒𝐡 οΏ½2𝑝

, βˆ’ 2𝑝

οΏ½

Area of βˆ†OAB = 12

|𝑂𝐴||𝑂𝐡|

= 12

οΏ½οΏ½(2𝑝)2 + (2𝑝)2οΏ½ οΏ½οΏ½οΏ½2𝑝

οΏ½2

+ οΏ½βˆ’2𝑝

οΏ½2

οΏ½

= 12

οΏ½π‘βˆš8οΏ½ οΏ½1𝑝 √8οΏ½

= 12

(8) = 4 units2

∴Area of βˆ†OAB is independent of p. (shown)

(iii) x = t + 1𝑑 …………………………(2)

y = t βˆ’ 1𝑑 …………………………(3)

(2) + (3) x + y = 2t

t = π‘₯+𝑦2

…………………………(4)

Sub (4) into (2)

x = π‘₯+𝑦2

+ 2π‘₯+𝑦

2x(x + y) = (x + y)2 + 4 2x2 + 2xy = x2 + 2xy + y2 + 4 4 + y2 = x2 x2 – y2 = 4

π’™πŸ

𝟐𝟐 βˆ’ π’šπŸ

𝟐𝟐 = 1

O

A

B

x

y

y = x

y = βˆ’x

(p2 + 1) x – (p2 – 1)y = 4p (arbitrary sketch for illustrative purpose)

Eliminate t, so that only x and y are left in the equation.

Graph of Hyperbola:

Equation: (π‘₯βˆ’β„Ž)2

π‘Ž2 βˆ’ (π‘¦βˆ’π‘˜)2

𝑏2 = 1 Center: (h, k) Oblique Asymptotes: 𝑦 = π‘˜ Β± 𝑏

π‘Ž(π‘₯ βˆ’ β„Ž)

OAβŠ₯OB

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Mathematics H2 (9740/01) version 2.1

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Using G.C. (refer to Appendix for detailed steps),

Asymptotes: y = x and y = βˆ’ x x-intercepts: (βˆ’2, 0) and (2, 0)

y = x y = βˆ’x y

x 0

(2, 0) (βˆ’2, 0)

𝐢:π‘₯2

22 βˆ’π‘¦2

22 = 1

y = x

y = βˆ’x

(βˆ’2, 0) (2, 0)

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Appendix: Detailed G. C. Steps (for those still trapped in G. C. limbo)

Q5 (ii): Sketching the Inverse of a Function

β†’ Ensure G. C. is in FUNC mode.

β†’ Plot f(x)

β†’ Plot fβˆ’1(x)

β†’ Plot f(x)

[SHIFT] [EXIT] [F6]

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Mathematics H2 (9740/01) version 2.1

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β†’ Plot fβˆ’1(x)

Q11: Sketching A Hyperbola

β†’ Enter Conics. β†’ Enter HYPERBOLA.

[F4]

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Q6 (i): Finding the Roots of a Function

Method I:Using Zero Values of Graphs

β†’ Define approximate bounds of x value to left/right of Ξ². β†’ Repeat steps for root Ξ³.

Method II: Using Solver

β†’Enter Solver (last item on MATH menu) β†’ Enter equation.

β†’ Enter suitable approximate value of x (i.e. x = 0) for root Ξ². β†’ Enter suitable approximate value of x (i.e. x = 2) for root Ξ³.

Method III: Using Poly Root Finder Application

β†’ Enter PlySmlt2

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Method I: Find Roots in Graph

Method II: Using Polynomials in Equation

Q6 (ii): Finding Region Bounded by Curve

Method I:Using β€œfnInt(β€œ Function

β†’ Key in lower/upper limits, expression and the integrating

variable (x).

Method II: Using Integration Function in Graph

β†’ Enter Ξ² and Ξ³ as the values for lower and upper limit

respectively.

[F5]

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Method I:Using Integration Function in Graph

Method II: Using Integration Function in MATHInput Mode β†’ Key in lower/upper limits and the expression.

[F5]

[SHIFT][MENU]

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Q7: Graph Sketching

β†’ Ensure G. C. is in FUNC mode.

[SHIFT] [EXIT] [F6]

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Q9 (iii): Finding the Range of Values in a Function

β†’ Enter expression

β†’ Enter X = 0 and X = 1to obtain the corresponding values of Y.

β†’ Enter X = 0 and X = 1to obtain the corresponding values of Y.

[F5]


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