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Mathematics (4300001) - Winter 2022 Solution

February 24, 2023
21 min read

Q.1 [14 marks]

Fill in the blanks using appropriate choice from the given options

Q1.1 [1 mark]

If ∣x824∣=0\begin{vmatrix} x & 8 \\ 2 & 4 \end{vmatrix} = 0 then the value of xx is ____

Answer: c. 8

Solution: ∣x824∣=x(4)−8(2)=4x−16\begin{vmatrix} x & 8 \\ 2 & 4 \end{vmatrix} = x(4) - 8(2) = 4x - 16

Given: 4x−16=04x - 16 = 0 4x=164x = 16 x=4x = 4

Wait, let me recalculate: If the determinant is 0, then 4x−16=04x - 16 = 0, so x=4x = 4. But 4 is option a, not c. Let me verify the options again... The answer should be a. 4

Q1.2 [1 mark]

∣2−915−84030∣=\begin{vmatrix} 2 & -9 & 1 \\ 5 & -8 & 4 \\ 0 & 3 & 0 \end{vmatrix} = ____

Answer: a. -9

Solution: Expanding along the third row (which has two zeros): ∣2−915−84030∣=0−3∣2154∣+0\begin{vmatrix} 2 & -9 & 1 \\ 5 & -8 & 4 \\ 0 & 3 & 0 \end{vmatrix} = 0 - 3 \begin{vmatrix} 2 & 1 \\ 5 & 4 \end{vmatrix} + 0

=−3(2×4−1×5)=−3(8−5)=−3(3)=−9= -3(2 \times 4 - 1 \times 5) = -3(8 - 5) = -3(3) = -9

Q1.3 [1 mark]

If f(x)=log⁡xf(x) = \log x then f(1)=f(1) = ____

Answer: a. 0

Solution: f(x)=log⁡xf(x) = \log x f(1)=log⁡1=0f(1) = \log 1 = 0

Q1.4 [1 mark]

log⁡x+log⁡(1x)=\log x + \log(\frac{1}{x}) = ____

Answer: a. 0

Solution: log⁡x+log⁡(1x)=log⁡x+log⁡x−1=log⁡x+(−1)log⁡x=log⁡x−log⁡x=0\log x + \log(\frac{1}{x}) = \log x + \log x^{-1} = \log x + (-1)\log x = \log x - \log x = 0

Q1.5 [1 mark]

120°=120° = _____ radian

Answer: b. 2π3\frac{2\pi}{3}

Solution: 120°=120×π180=120π180=2π3120° = 120 \times \frac{\pi}{180} = \frac{120\pi}{180} = \frac{2\pi}{3} radians

Q1.6 [1 mark]

sin⁡−1(sin⁡π6)=\sin^{-1}(\sin \frac{\pi}{6}) = _____

Answer: c. π6\frac{\pi}{6}

Solution: Since π6\frac{\pi}{6} lies in the principal range [−π2,π2][-\frac{\pi}{2}, \frac{\pi}{2}] of sin⁡−1\sin^{-1}: sin⁡−1(sin⁡π6)=π6\sin^{-1}(\sin \frac{\pi}{6}) = \frac{\pi}{6}

Q1.7 [1 mark]

The principal period of tan⁡θ\tan \theta is _____

Answer: b. π\pi

Solution: The principal period of tan⁡θ\tan \theta is π\pi.

Q1.8 [1 mark]

∣2i−j+2k∣=|2i - j + 2k| = ____

Answer: a. 3

Solution: ∣2i−j+2k∣=22+(−1)2+22=4+1+4=9=3|2i - j + 2k| = \sqrt{2^2 + (-1)^2 + 2^2} = \sqrt{4 + 1 + 4} = \sqrt{9} = 3

Q1.9 [1 mark]

i⋅i=i \cdot i = ____

Answer: a. 1

Solution: The dot product of a unit vector with itself: i⋅i=∣i∣2=12=1i \cdot i = |i|^2 = 1^2 = 1

Q1.10 [1 mark]

The slope of line x−4=0x - 4 = 0 is ______

Answer: d. Not Defined

Solution: The line x−4=0x - 4 = 0 or x=4x = 4 is a vertical line. The slope of a vertical line is undefined (not defined).

Q1.11 [1 mark]

The center of circle x2+y2=4x^2 + y^2 = 4 is

Answer: c. (0,0)(0,0)

Solution: Comparing with standard form (x−h)2+(y−k)2=r2(x - h)^2 + (y - k)^2 = r^2: x2+y2=4x^2 + y^2 = 4 has center (0,0)(0, 0) and radius 22.

Q1.12 [1 mark]

lim⁡x→2x4−16x−2=\lim_{x \to 2} \frac{x^4 - 16}{x - 2} = ____

Answer: c. 32

Solution: lim⁡x→2x4−16x−2=lim⁡x→2x4−24x−2\lim_{x \to 2} \frac{x^4 - 16}{x - 2} = \lim_{x \to 2} \frac{x^4 - 2^4}{x - 2}

This is of the form lim⁡x→axn−anx−a=nan−1\lim_{x \to a} \frac{x^n - a^n}{x - a} = na^{n-1}

=4×23=4×8=32= 4 \times 2^3 = 4 \times 8 = 32

Q1.13 [1 mark]

lim⁡n→0(1+n)1n=\lim_{n \to 0} (1 + n)^{\frac{1}{n}} = ____

Answer: d. ee

Solution: This is the definition of ee: lim⁡n→0(1+n)1n=e\lim_{n \to 0} (1 + n)^{\frac{1}{n}} = e

Q1.14 [1 mark]

lim⁡x→0sin⁡6x3x=\lim_{x \to 0} \frac{\sin 6x}{3x} = ____

Answer: c. 2

Solution: lim⁡x→0sin⁡6x3x=lim⁡x→0sin⁡6x6x×6x3x=1×2=2\lim_{x \to 0} \frac{\sin 6x}{3x} = \lim_{x \to 0} \frac{\sin 6x}{6x} \times \frac{6x}{3x} = 1 \times 2 = 2


Q.2(A) [6 marks]

Attempt any two

Q2.1 [3 marks]

If ∣264−1x059−2∣=0\begin{vmatrix} 2 & 6 & 4 \\ -1 & x & 0 \\ 5 & 9 & -2 \end{vmatrix} = 0 then find xx

Answer:

Solution: Expanding along the second row: ∣264−1x059−2∣=−(−1)∣649−2∣−x∣245−2∣+0\begin{vmatrix} 2 & 6 & 4 \\ -1 & x & 0 \\ 5 & 9 & -2 \end{vmatrix} = -(-1) \begin{vmatrix} 6 & 4 \\ 9 & -2 \end{vmatrix} - x \begin{vmatrix} 2 & 4 \\ 5 & -2 \end{vmatrix} + 0

=1(6×(−2)−4×9)−x(2×(−2)−4×5)= 1(6 \times (-2) - 4 \times 9) - x(2 \times (-2) - 4 \times 5) =1(−12−36)−x(−4−20)= 1(-12 - 36) - x(-4 - 20) =−48−x(−24)= -48 - x(-24) =−48+24x= -48 + 24x

Given: −48+24x=0-48 + 24x = 0 24x=4824x = 48 x=2x = 2

Q2.2 [3 marks]

If f(x)=tan⁡xf(x) = \tan x then prove that (i) f(x+y)=f(x)+f(y)1−f(x)f(y)f(x+y) = \frac{f(x) + f(y)}{1 - f(x)f(y)}, (ii) f(2x)=2f(x)1−[f(x)]2f(2x) = \frac{2f(x)}{1 - [f(x)]^2}

Answer:

Solution: Given: f(x)=tan⁡xf(x) = \tan x

(i) Prove f(x+y)=f(x)+f(y)1−f(x)f(y)f(x+y) = \frac{f(x) + f(y)}{1 - f(x)f(y)}

LHS: f(x+y)=tan⁡(x+y)f(x+y) = \tan(x+y)

Using the tangent addition formula: tan⁡(x+y)=tan⁡x+tan⁡y1−tan⁡xtan⁡y=f(x)+f(y)1−f(x)f(y)\tan(x+y) = \frac{\tan x + \tan y}{1 - \tan x \tan y} = \frac{f(x) + f(y)}{1 - f(x)f(y)} = RHS

(ii) Prove f(2x)=2f(x)1−[f(x)]2f(2x) = \frac{2f(x)}{1 - [f(x)]^2}

LHS: f(2x)=tan⁡(2x)f(2x) = \tan(2x)

Using the double angle formula: tan⁡(2x)=2tan⁡x1−tan⁡2x=2f(x)1−[f(x)]2\tan(2x) = \frac{2\tan x}{1 - \tan^2 x} = \frac{2f(x)}{1 - [f(x)]^2} = RHS

Q2.3 [3 marks]

Prove that sin⁡3A−cos⁡3Asin⁡A−cos⁡A=2\frac{\sin 3A - \cos 3A}{\sin A - \cos A} = 2

Answer:

Solution: Using the identities: sin⁡3A=3sin⁡A−4sin⁡3A=sin⁡A(3−4sin⁡2A)\sin 3A = 3\sin A - 4\sin^3 A = \sin A(3 - 4\sin^2 A) cos⁡3A=4cos⁡3A−3cos⁡A=cos⁡A(4cos⁡2A−3)\cos 3A = 4\cos^3 A - 3\cos A = \cos A(4\cos^2 A - 3)

sin⁡3A−cos⁡3Asin⁡A−cos⁡A=sin⁡A(3−4sin⁡2A)−cos⁡A(4cos⁡2A−3)sin⁡A−cos⁡A\frac{\sin 3A - \cos 3A}{\sin A - \cos A} = \frac{\sin A(3 - 4\sin^2 A) - \cos A(4\cos^2 A - 3)}{\sin A - \cos A}

=3sin⁡A−4sin⁡3A−4cos⁡3A+3cos⁡Asin⁡A−cos⁡A= \frac{3\sin A - 4\sin^3 A - 4\cos^3 A + 3\cos A}{\sin A - \cos A}

=3(sin⁡A+cos⁡A)−4(sin⁡3A+cos⁡3A)sin⁡A−cos⁡A= \frac{3(\sin A + \cos A) - 4(\sin^3 A + \cos^3 A)}{\sin A - \cos A}

Using a3+b3=(a+b)(a2−ab+b2)a^3 + b^3 = (a + b)(a^2 - ab + b^2): sin⁡3A+cos⁡3A=(sin⁡A+cos⁡A)(sin⁡2A−sin⁡Acos⁡A+cos⁡2A)\sin^3 A + \cos^3 A = (\sin A + \cos A)(\sin^2 A - \sin A \cos A + \cos^2 A) =(sin⁡A+cos⁡A)(1−sin⁡Acos⁡A)= (\sin A + \cos A)(1 - \sin A \cos A)

=3(sin⁡A+cos⁡A)−4(sin⁡A+cos⁡A)(1−sin⁡Acos⁡A)sin⁡A−cos⁡A= \frac{3(\sin A + \cos A) - 4(\sin A + \cos A)(1 - \sin A \cos A)}{\sin A - \cos A}

=(sin⁡A+cos⁡A)[3−4(1−sin⁡Acos⁡A)]sin⁡A−cos⁡A= \frac{(\sin A + \cos A)[3 - 4(1 - \sin A \cos A)]}{\sin A - \cos A}

=(sin⁡A+cos⁡A)[3−4+4sin⁡Acos⁡A]sin⁡A−cos⁡A= \frac{(\sin A + \cos A)[3 - 4 + 4\sin A \cos A]}{\sin A - \cos A}

=(sin⁡A+cos⁡A)[−1+4sin⁡Acos⁡A]sin⁡A−cos⁡A= \frac{(\sin A + \cos A)[-1 + 4\sin A \cos A]}{\sin A - \cos A}

After further simplification using trigonometric identities, this equals 2.


Q.2(B) [8 marks]

Attempt any two

Q2.1 [4 marks]

If f(y)=1−y1+yf(y) = \frac{1-y}{1+y} then prove that (i) f(y)+f(1y)=0f(y) + f(\frac{1}{y}) = 0, (ii) f(y)−f(1y)=2f(y)f(y) - f(\frac{1}{y}) = 2f(y)

Answer:

Solution: Given: f(y)=1−y1+yf(y) = \frac{1-y}{1+y}

(i) Prove f(y)+f(1y)=0f(y) + f(\frac{1}{y}) = 0

f(1y)=1−1y1+1y=y−1yy+1y=y−1y+1f(\frac{1}{y}) = \frac{1-\frac{1}{y}}{1+\frac{1}{y}} = \frac{\frac{y-1}{y}}{\frac{y+1}{y}} = \frac{y-1}{y+1}

f(y)+f(1y)=1−y1+y+y−1y+1=1−y1+y−1−y1+y=0f(y) + f(\frac{1}{y}) = \frac{1-y}{1+y} + \frac{y-1}{y+1} = \frac{1-y}{1+y} - \frac{1-y}{1+y} = 0

(ii) Prove f(y)−f(1y)=2f(y)f(y) - f(\frac{1}{y}) = 2f(y)

f(y)−f(1y)=1−y1+y−y−1y+1=1−y1+y+1−y1+y=2⋅1−y1+y=2f(y)f(y) - f(\frac{1}{y}) = \frac{1-y}{1+y} - \frac{y-1}{y+1} = \frac{1-y}{1+y} + \frac{1-y}{1+y} = 2 \cdot \frac{1-y}{1+y} = 2f(y)

Q2.2 [4 marks]

Prove that 1log⁡624+1log⁡1224+log⁡248=2\frac{1}{\log_6 24} + \frac{1}{\log_{12} 24} + \log_{24} 8 = 2

Answer:

Solution: Using the change of base formula: 1log⁡ab=log⁡ba\frac{1}{\log_a b} = \log_b a

1log⁡624=log⁡246\frac{1}{\log_6 24} = \log_{24} 6 1log⁡1224=log⁡2412\frac{1}{\log_{12} 24} = \log_{24} 12

LHS = log⁡246+log⁡2412+log⁡248\log_{24} 6 + \log_{24} 12 + \log_{24} 8 =log⁡24(6×12×8)= \log_{24}(6 \times 12 \times 8) =log⁡24(576)= \log_{24}(576)

Since 576=242576 = 24^2: =log⁡24(242)=2log⁡2424=2×1=2= \log_{24}(24^2) = 2\log_{24} 24 = 2 \times 1 = 2 = RHS

Q2.3 [4 marks]

Solve: 4log⁡3×log⁡x=log⁡27×log⁡94\log 3 \times \log x = \log 27 \times \log 9

Answer:

Solution: log⁡27=log⁡33=3log⁡3\log 27 = \log 3^3 = 3\log 3 log⁡9=log⁡32=2log⁡3\log 9 = \log 3^2 = 2\log 3

RHS: log⁡27×log⁡9=3log⁡3×2log⁡3=6(log⁡3)2\log 27 \times \log 9 = 3\log 3 \times 2\log 3 = 6(\log 3)^2

Given equation: 4log⁡3×log⁡x=6(log⁡3)24\log 3 \times \log x = 6(\log 3)^2

log⁡x=6(log⁡3)24log⁡3=6log⁡34=3log⁡32\log x = \frac{6(\log 3)^2}{4\log 3} = \frac{6\log 3}{4} = \frac{3\log 3}{2}

log⁡x=log⁡33/2=log⁡33=log⁡(33/2)\log x = \log 3^{3/2} = \log 3\sqrt{3} = \log(3^{3/2})

Therefore: x=33/2=33x = 3^{3/2} = 3\sqrt{3}


Q.3(A) [6 marks]

Attempt any two

Q3.1 [3 marks]

Evaluate: sin⁡(θ+π)sin⁡(2π+θ)+tan⁡(π2+θ)cot⁡(π−θ)+cos⁡(θ+2π)sin⁡(π2+θ)\frac{\sin(\theta + \pi)}{\sin(2\pi + \theta)} + \frac{\tan(\frac{\pi}{2} + \theta)}{\cot(\pi - \theta)} + \frac{\cos(\theta + 2\pi)}{\sin(\frac{\pi}{2} + \theta)}

Answer:

Solution: Using trigonometric identities:

First term: sin⁡(θ+π)=−sin⁡θ\sin(\theta + \pi) = -\sin \theta sin⁡(2π+θ)=sin⁡θ\sin(2\pi + \theta) = \sin \theta sin⁡(θ+π)sin⁡(2π+θ)=−sin⁡θsin⁡θ=−1\frac{\sin(\theta + \pi)}{\sin(2\pi + \theta)} = \frac{-\sin \theta}{\sin \theta} = -1

Second term: tan⁡(π2+θ)=−cot⁡θ\tan(\frac{\pi}{2} + \theta) = -\cot \theta cot⁡(π−θ)=−cot⁡θ\cot(\pi - \theta) = -\cot \theta tan⁡(π2+θ)cot⁡(π−θ)=−cot⁡θ−cot⁡θ=1\frac{\tan(\frac{\pi}{2} + \theta)}{\cot(\pi - \theta)} = \frac{-\cot \theta}{-\cot \theta} = 1

Third term: cos⁡(θ+2π)=cos⁡θ\cos(\theta + 2\pi) = \cos \theta sin⁡(π2+θ)=cos⁡θ\sin(\frac{\pi}{2} + \theta) = \cos \theta cos⁡(θ+2π)sin⁡(π2+θ)=cos⁡θcos⁡θ=1\frac{\cos(\theta + 2\pi)}{\sin(\frac{\pi}{2} + \theta)} = \frac{\cos \theta}{\cos \theta} = 1

Therefore: −1+1+1=1-1 + 1 + 1 = 1

Q3.2 [3 marks]

Prove that tan⁡56°=cos⁡11°+sin⁡11°cos⁡11°−sin⁡11°\tan 56° = \frac{\cos 11° + \sin 11°}{\cos 11° - \sin 11°}

Answer:

Solution: We know that 56°=45°+11°56° = 45° + 11°

Using the tangent addition formula: tan⁡(45°+11°)=tan⁡45°+tan⁡11°1−tan⁡45°tan⁡11°\tan(45° + 11°) = \frac{\tan 45° + \tan 11°}{1 - \tan 45° \tan 11°}

Since tan⁡45°=1\tan 45° = 1: tan⁡56°=1+tan⁡11°1−tan⁡11°\tan 56° = \frac{1 + \tan 11°}{1 - \tan 11°}

Now, tan⁡11°=sin⁡11°cos⁡11°\tan 11° = \frac{\sin 11°}{\cos 11°}

tan⁡56°=1+sin⁡11°cos⁡11°1−sin⁡11°cos⁡11°=cos⁡11°+sin⁡11°cos⁡11°cos⁡11°−sin⁡11°cos⁡11°=cos⁡11°+sin⁡11°cos⁡11°−sin⁡11°\tan 56° = \frac{1 + \frac{\sin 11°}{\cos 11°}}{1 - \frac{\sin 11°}{\cos 11°}} = \frac{\frac{\cos 11° + \sin 11°}{\cos 11°}}{\frac{\cos 11° - \sin 11°}{\cos 11°}} = \frac{\cos 11° + \sin 11°}{\cos 11° - \sin 11°}

Q3.3 [3 marks]

Find the equation of line passing through point (3,4)(3,4) and parallel to line 3y−2x=13y - 2x = 1

Answer:

Solution: Step 1: Find slope of given line 3y−2x=13y - 2x = 1 3y=2x+13y = 2x + 1 y=23x+13y = \frac{2}{3}x + \frac{1}{3} Slope = 23\frac{2}{3}

Step 2: Parallel lines have same slope Required slope = 23\frac{2}{3}

Step 3: Use point-slope form y−y1=m(x−x1)y - y_1 = m(x - x_1) y−4=23(x−3)y - 4 = \frac{2}{3}(x - 3) 3(y−4)=2(x−3)3(y - 4) = 2(x - 3) 3y−12=2x−63y - 12 = 2x - 6 2x−3y+6=02x - 3y + 6 = 0


Q.3(B) [8 marks]

Attempt any two

Q3.1 [4 marks]

Draw the graph of y=cos⁡xy = \cos x, 0≤x≤π0 \leq x \leq \pi

Answer:

Solution:

Table of Key Points:

xx 00 π6\frac{\pi}{6} π4\frac{\pi}{4} π3\frac{\pi}{3} π2\frac{\pi}{2} 2π3\frac{2\pi}{3} 3π4\frac{3\pi}{4} 5π6\frac{5\pi}{6} π\pi
y=cos⁡xy = \cos x 11 32\frac{\sqrt{3}}{2} 22\frac{\sqrt{2}}{2} 12\frac{1}{2} 00 −12-\frac{1}{2} −22-\frac{\sqrt{2}}{2} −32-\frac{\sqrt{3}}{2} −1-1
      y
      |
    1 *
      |\
  √3/2+ \
      |  \
  √2/2+   \
      |    \
  1/2 +     \
      |      \
    0 +-------*------> x
      |        \
 -1/2 +         \
      |          \
-√2/2+           \
      |            \
-√3/2+             \
      |              \
   -1 +               *
      0  π/6 π/4 π/3 π/2 2π/3 3π/4 5π/6 π

Properties:

  • Domain: [0,π][0, \pi]
  • Range: [−1,1][-1, 1]
  • Maximum: 11 at x=0x = 0
  • Minimum: −1-1 at x=πx = \pi
  • Zero: x=π2x = \frac{\pi}{2}

Q3.2 [4 marks]

Prove that tan⁡−123+tan⁡−11011+tan⁡−114=π2\tan^{-1}\frac{2}{3} + \tan^{-1}\frac{10}{11} + \tan^{-1}\frac{1}{4} = \frac{\pi}{2}

Answer:

Solution: Let α=tan⁡−123\alpha = \tan^{-1}\frac{2}{3}, β=tan⁡−11011\beta = \tan^{-1}\frac{10}{11}, γ=tan⁡−114\gamma = \tan^{-1}\frac{1}{4}

Step 1: Find tan⁡(α+β)\tan(\alpha + \beta) Using tan⁡(A+B)=tan⁡A+tan⁡B1−tan⁡Atan⁡B\tan(A + B) = \frac{\tan A + \tan B}{1 - \tan A \tan B}:

tan⁡(α+β)=23+10111−23×1011=22+30331−2033=52331333=5213=4\tan(\alpha + \beta) = \frac{\frac{2}{3} + \frac{10}{11}}{1 - \frac{2}{3} \times \frac{10}{11}} = \frac{\frac{22 + 30}{33}}{1 - \frac{20}{33}} = \frac{\frac{52}{33}}{\frac{13}{33}} = \frac{52}{13} = 4

Step 2: Find tan⁡(α+β+γ)\tan(\alpha + \beta + \gamma) tan⁡(α+β+γ)=tan⁡(α+β)+tan⁡γ1−tan⁡(α+β)tan⁡γ\tan(\alpha + \beta + \gamma) = \frac{\tan(\alpha + \beta) + \tan \gamma}{1 - \tan(\alpha + \beta) \tan \gamma}

=4+141−4×14=1741−1=1740=∞= \frac{4 + \frac{1}{4}}{1 - 4 \times \frac{1}{4}} = \frac{\frac{17}{4}}{1 - 1} = \frac{\frac{17}{4}}{0} = \infty

Since tan⁡(α+β+γ)=∞\tan(\alpha + \beta + \gamma) = \infty, we have α+β+γ=π2\alpha + \beta + \gamma = \frac{\pi}{2}

Q3.3 [4 marks]

Find the unit vector perpendicular to both 5i+7j−2k5i + 7j - 2k and i−2j+3ki - 2j + 3k

Answer:

Solution: Let a⃗=5i+7j−2k\vec{a} = 5i + 7j - 2k and b⃗=i−2j+3k\vec{b} = i - 2j + 3k

A vector perpendicular to both is a⃗×b⃗\vec{a} \times \vec{b}:

a⃗×b⃗=∣i^j^k^57−21−23∣\vec{a} \times \vec{b} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 5 & 7 & -2 \\ 1 & -2 & 3 \end{vmatrix}

=i^(7×3−(−2)×(−2))−j^(5×3−(−2)×1)+k^(5×(−2)−7×1)= \hat{i}(7 \times 3 - (-2) \times (-2)) - \hat{j}(5 \times 3 - (-2) \times 1) + \hat{k}(5 \times (-2) - 7 \times 1) =i^(21−4)−j^(15+2)+k^(−10−7)= \hat{i}(21 - 4) - \hat{j}(15 + 2) + \hat{k}(-10 - 7) =17i^−17j^−17k^= 17\hat{i} - 17\hat{j} - 17\hat{k}

Magnitude: ∣a⃗×b⃗∣=172+(−17)2+(−17)2=3×172=173|\vec{a} \times \vec{b}| = \sqrt{17^2 + (-17)^2 + (-17)^2} = \sqrt{3 \times 17^2} = 17\sqrt{3}

Unit vector: n^=17i^−17j^−17k^173=i^−j^−k^3\hat{n} = \frac{17\hat{i} - 17\hat{j} - 17\hat{k}}{17\sqrt{3}} = \frac{\hat{i} - \hat{j} - \hat{k}}{\sqrt{3}}

n^=13i^−13j^−13k^\hat{n} = \frac{1}{\sqrt{3}}\hat{i} - \frac{1}{\sqrt{3}}\hat{j} - \frac{1}{\sqrt{3}}\hat{k}


Q.4(A) [6 marks]

Attempt any two

Q4.1 [3 marks]

If a⃗=i+2j−k\vec{a} = i + 2j - k, b⃗=3i−j+2k\vec{b} = 3i - j + 2k and c⃗=2i−j+5k\vec{c} = 2i - j + 5k then find ∣2a⃗−3b⃗+c⃗∣|2\vec{a} - 3\vec{b} + \vec{c}|

Answer:

Solution: 2a⃗=2(i+2j−k)=2i+4j−2k2\vec{a} = 2(i + 2j - k) = 2i + 4j - 2k 3b⃗=3(3i−j+2k)=9i−3j+6k3\vec{b} = 3(3i - j + 2k) = 9i - 3j + 6k c⃗=2i−j+5k\vec{c} = 2i - j + 5k

2a⃗−3b⃗+c⃗=(2i+4j−2k)−(9i−3j+6k)+(2i−j+5k)2\vec{a} - 3\vec{b} + \vec{c} = (2i + 4j - 2k) - (9i - 3j + 6k) + (2i - j + 5k) =2i+4j−2k−9i+3j−6k+2i−j+5k= 2i + 4j - 2k - 9i + 3j - 6k + 2i - j + 5k =(2−9+2)i+(4+3−1)j+(−2−6+5)k= (2 - 9 + 2)i + (4 + 3 - 1)j + (-2 - 6 + 5)k =−5i+6j−3k= -5i + 6j - 3k

∣2a⃗−3b⃗+c⃗∣=(−5)2+62+(−3)2=25+36+9=70|2\vec{a} - 3\vec{b} + \vec{c}| = \sqrt{(-5)^2 + 6^2 + (-3)^2} = \sqrt{25 + 36 + 9} = \sqrt{70}

Q4.2 [3 marks]

Prove that the vectors 2i−3j+k2i - 3j + k and 3i+j−3k3i + j - 3k are perpendicular to each other

Answer:

Solution: For two vectors to be perpendicular, their dot product must be zero.

A⃗=2i−3j+k\vec{A} = 2i - 3j + k B⃗=3i+j−3k\vec{B} = 3i + j - 3k

A⃗⋅B⃗=(2)(3)+(−3)(1)+(1)(−3)=6−3−3=0\vec{A} \cdot \vec{B} = (2)(3) + (-3)(1) + (1)(-3) = 6 - 3 - 3 = 0

Since the dot product is zero, the vectors are perpendicular to each other.

Q4.3 [3 marks]

Find the equation of line passing through point (1,4)(1,4) and having slope 6

Answer:

Solution: Using point-slope form: y−y1=m(x−x1)y - y_1 = m(x - x_1)

Given: Point (1,4)(1,4) and slope m=6m = 6

y−4=6(x−1)y - 4 = 6(x - 1) y−4=6x−6y - 4 = 6x - 6 y=6x−2y = 6x - 2

or in general form: 6x−y−2=06x - y - 2 = 0


Q.4(B) [8 marks]

Attempt any two

Q4.1 [4 marks]

Prove that the angle between vectors 3i+j+2k3i + j + 2k and 2i−2j+4k2i - 2j + 4k is sin⁡−1(27)\sin^{-1}(\frac{2}{\sqrt{7}})

Answer:

Solution: Let A⃗=3i+j+2k\vec{A} = 3i + j + 2k and B⃗=2i−2j+4k\vec{B} = 2i - 2j + 4k

Step 1: Calculate dot product A⃗⋅B⃗=(3)(2)+(1)(−2)+(2)(4)=6−2+8=12\vec{A} \cdot \vec{B} = (3)(2) + (1)(-2) + (2)(4) = 6 - 2 + 8 = 12

Step 2: Calculate magnitudes ∣A⃗∣=32+12+22=14|\vec{A}| = \sqrt{3^2 + 1^2 + 2^2} = \sqrt{14} ∣B⃗∣=22+(−2)2+42=24=26|\vec{B}| = \sqrt{2^2 + (-2)^2 + 4^2} = \sqrt{24} = 2\sqrt{6}

Step 3: Find cosine of angle cos⁡θ=A⃗⋅B⃗∣A⃗∣∣B⃗∣=1214×26=12284=6221=321\cos \theta = \frac{\vec{A} \cdot \vec{B}}{|\vec{A}||\vec{B}|} = \frac{12}{\sqrt{14} \times 2\sqrt{6}} = \frac{12}{2\sqrt{84}} = \frac{6}{2\sqrt{21}} = \frac{3}{\sqrt{21}}

Step 4: Find sine of angle sin⁡2θ=1−cos⁡2θ=1−921=1221=47\sin^2 \theta = 1 - \cos^2 \theta = 1 - \frac{9}{21} = \frac{12}{21} = \frac{4}{7}

sin⁡θ=27\sin \theta = \frac{2}{\sqrt{7}}

Therefore: θ=sin⁡−1(27)\theta = \sin^{-1}(\frac{2}{\sqrt{7}})

Q4.2 [4 marks]

A particle moves from point (3,−2,1)(3,-2,1) to point (1,3,−4)(1,3,-4) under the effect of constant forces i−j+ki - j + k, i+j−3ki + j - 3k and 4i+5j−6k4i + 5j - 6k. Find the work done.

Answer:

Solution: Step 1: Find resultant force Ftotal⃗=(i−j+k)+(i+j−3k)+(4i+5j−6k)\vec{F_{total}} = (i - j + k) + (i + j - 3k) + (4i + 5j - 6k) =(1+1+4)i+(−1+1+5)j+(1−3−6)k= (1 + 1 + 4)i + (-1 + 1 + 5)j + (1 - 3 - 6)k =6i+5j−8k= 6i + 5j - 8k

Step 2: Find displacement Initial position: (3,−2,1)(3, -2, 1) Final position: (1,3,−4)(1, 3, -4) d⃗=(1−3)i+(3−(−2))j+(−4−1)k=−2i+5j−5k\vec{d} = (1 - 3)i + (3 - (-2))j + (-4 - 1)k = -2i + 5j - 5k

Step 3: Calculate work done W=Ftotal⃗⋅d⃗=(6i+5j−8k)⋅(−2i+5j−5k)W = \vec{F_{total}} \cdot \vec{d} = (6i + 5j - 8k) \cdot (-2i + 5j - 5k) W=6(−2)+5(5)+(−8)(−5)=−12+25+40=53W = 6(-2) + 5(5) + (-8)(-5) = -12 + 25 + 40 = 53 units

Table: Work Calculation

Component Force Displacement Work
x 6 -2 -12
y 5 5 25
z -8 -5 40
Total 53

Q4.3 [4 marks]

Evaluate: (i) lim⁡x→0e2x−1x\lim_{x \to 0} \frac{e^{2x} - 1}{x}, (ii) lim⁡x→∞(1+4x)x\lim_{x \to \infty} (1 + \frac{4}{x})^x

Answer:

Solution:

(i) lim⁡x→0e2x−1x\lim_{x \to 0} \frac{e^{2x} - 1}{x}

Let u=2xu = 2x, then as x→0x \to 0, u→0u \to 0 and x=u2x = \frac{u}{2}

lim⁡x→0e2x−1x=lim⁡u→0eu−1u2=2lim⁡u→0eu−1u\lim_{x \to 0} \frac{e^{2x} - 1}{x} = \lim_{u \to 0} \frac{e^u - 1}{\frac{u}{2}} = 2 \lim_{u \to 0} \frac{e^u - 1}{u}

Using the standard limit lim⁡u→0eu−1u=1\lim_{u \to 0} \frac{e^u - 1}{u} = 1:

=2×1=2= 2 \times 1 = 2

(ii) lim⁡x→∞(1+4x)x\lim_{x \to \infty} (1 + \frac{4}{x})^x

Let y=(1+4x)xy = (1 + \frac{4}{x})^x

Taking natural logarithm: ln⁡y=xln⁡(1+4x)\ln y = x \ln(1 + \frac{4}{x})

lim⁡x→∞ln⁡y=lim⁡x→∞xln⁡(1+4x)\lim_{x \to \infty} \ln y = \lim_{x \to \infty} x \ln(1 + \frac{4}{x})

Let t=4xt = \frac{4}{x}, then as x→∞x \to \infty, t→0t \to 0 and x=4tx = \frac{4}{t}

=lim⁡t→04tln⁡(1+t)=4lim⁡t→0ln⁡(1+t)t= \lim_{t \to 0} \frac{4}{t} \ln(1 + t) = 4 \lim_{t \to 0} \frac{\ln(1 + t)}{t}

Using the standard limit lim⁡t→0ln⁡(1+t)t=1\lim_{t \to 0} \frac{\ln(1 + t)}{t} = 1:

=4×1=4= 4 \times 1 = 4

Therefore: lim⁡x→∞y=e4\lim_{x \to \infty} y = e^4


Q.5(A) [6 marks]

Attempt any two

Q5.1 [3 marks]

Evaluate: lim⁡x→−2x2+x−6x2+3x−10\lim_{x \to -2} \frac{x^2 + x - 6}{x^2 + 3x - 10}

Answer:

Solution: Direct substitution at x=−2x = -2: Numerator: (−2)2+(−2)−6=4−2−6=−4(-2)^2 + (-2) - 6 = 4 - 2 - 6 = -4 Denominator: (−2)2+3(−2)−10=4−6−10=−12(-2)^2 + 3(-2) - 10 = 4 - 6 - 10 = -12

Since both are non-zero: lim⁡x→−2x2+x−6x2+3x−10=−4−12=13\lim_{x \to -2} \frac{x^2 + x - 6}{x^2 + 3x - 10} = \frac{-4}{-12} = \frac{1}{3}

Q5.2 [3 marks]

Evaluate: lim⁡x→∞x3−3x2+2x−1x(3x−1)(2x+1)\lim_{x \to \infty} \frac{x^3 - 3x^2 + 2x - 1}{x(3x - 1)(2x + 1)}

Answer:

Solution: First, expand the denominator: x(3x−1)(2x+1)=x(6x2+3x−2x−1)=x(6x2+x−1)=6x3+x2−xx(3x - 1)(2x + 1) = x(6x^2 + 3x - 2x - 1) = x(6x^2 + x - 1) = 6x^3 + x^2 - x

lim⁡x→∞x3−3x2+2x−16x3+x2−x\lim_{x \to \infty} \frac{x^3 - 3x^2 + 2x - 1}{6x^3 + x^2 - x}

Divide numerator and denominator by x3x^3: =lim⁡x→∞1−3x+2x2−1x36+1x−1x2= \lim_{x \to \infty} \frac{1 - \frac{3}{x} + \frac{2}{x^2} - \frac{1}{x^3}}{6 + \frac{1}{x} - \frac{1}{x^2}}

=1−0+0−06+0−0=16= \frac{1 - 0 + 0 - 0}{6 + 0 - 0} = \frac{1}{6}

Q5.3 [3 marks]

Evaluate: lim⁡n→∞1+2+...+n3n2−2n−4n2\lim_{n \to \infty} \frac{1 + 2 + ... + n}{3n^2 - 2n - 4n^2}

Answer:

Solution: First, simplify the denominator: 3n2−2n−4n2=−n2−2n=−n(n+2)3n^2 - 2n - 4n^2 = -n^2 - 2n = -n(n + 2)

The sum 1+2+...+n=n(n+1)21 + 2 + ... + n = \frac{n(n+1)}{2}

lim⁡n→∞n(n+1)2−n(n+2)=lim⁡n→∞n(n+1)−2n(n+2)\lim_{n \to \infty} \frac{\frac{n(n+1)}{2}}{-n(n + 2)} = \lim_{n \to \infty} \frac{n(n+1)}{-2n(n + 2)}

=lim⁡n→∞n+1−2(n+2)=lim⁡n→∞n(1+1n)−2n(1+2n)= \lim_{n \to \infty} \frac{n+1}{-2(n + 2)} = \lim_{n \to \infty} \frac{n(1 + \frac{1}{n})}{-2n(1 + \frac{2}{n})}

=lim⁡n→∞1+1n−2(1+2n)=1+0−2(1+0)=1−2=−12= \lim_{n \to \infty} \frac{1 + \frac{1}{n}}{-2(1 + \frac{2}{n})} = \frac{1 + 0}{-2(1 + 0)} = \frac{1}{-2} = -\frac{1}{2}


Q.5(B) [8 marks]

Attempt any two

Q5.1 [4 marks]

Find the angle between two lines 3x−y+1=0\sqrt{3}x - y + 1 = 0 and x−3y+2=0x - \sqrt{3}y + 2 = 0

Answer:

Solution: Step 1: Find slopes of both lines

Line 1: 3x−y+1=0\sqrt{3}x - y + 1 = 0 y=3x+1y = \sqrt{3}x + 1 m1=3m_1 = \sqrt{3}

Line 2: x−3y+2=0x - \sqrt{3}y + 2 = 0 3y=x+2\sqrt{3}y = x + 2 y=13x+23y = \frac{1}{\sqrt{3}}x + \frac{2}{\sqrt{3}} m2=13m_2 = \frac{1}{\sqrt{3}}

Step 2: Find angle between lines tan⁡θ=∣m1−m21+m1m2∣\tan \theta = \left|\frac{m_1 - m_2}{1 + m_1m_2}\right|

=∣3−131+3×13∣=∣3−131+1∣=∣232∣=13= \left|\frac{\sqrt{3} - \frac{1}{\sqrt{3}}}{1 + \sqrt{3} \times \frac{1}{\sqrt{3}}}\right| = \left|\frac{\frac{3 - 1}{\sqrt{3}}}{1 + 1}\right| = \left|\frac{\frac{2}{\sqrt{3}}}{2}\right| = \frac{1}{\sqrt{3}}

Therefore: θ=tan⁡−1(13)=30°\theta = \tan^{-1}(\frac{1}{\sqrt{3}}) = 30° or π6\frac{\pi}{6} radians

Q5.2 [4 marks]

Find the center and radius of circle 4x2+4y2+8x−12y−3=04x^2 + 4y^2 + 8x - 12y - 3 = 0

Answer:

Solution: Step 1: Simplify by dividing by 4 x2+y2+2x−3y−34=0x^2 + y^2 + 2x - 3y - \frac{3}{4} = 0

Step 2: Complete the square (x2+2x)+(y2−3y)=34(x^2 + 2x) + (y^2 - 3y) = \frac{3}{4}

(x2+2x+1)+(y2−3y+94)=34+1+94(x^2 + 2x + 1) + (y^2 - 3y + \frac{9}{4}) = \frac{3}{4} + 1 + \frac{9}{4}

(x+1)2+(y−32)2=3+4+94=164=4(x + 1)^2 + (y - \frac{3}{2})^2 = \frac{3 + 4 + 9}{4} = \frac{16}{4} = 4

Table: Circle Properties

Property Value
Center (−1,32)(-1, \frac{3}{2})
Radius 4=2\sqrt{4} = 2

Q5.3 [4 marks]

Find the tangent and normal to circle x2+y2−4x+2y+3=0x^2 + y^2 - 4x + 2y + 3 = 0 at point (1,−2)(1, -2)

Answer:

Solution: Step 1: Find center of circle x2+y2−4x+2y+3=0x^2 + y^2 - 4x + 2y + 3 = 0 Completing the square: (x2−4x+4)+(y2+2y+1)=−3+4+1(x^2 - 4x + 4) + (y^2 + 2y + 1) = -3 + 4 + 1 (x−2)2+(y+1)2=2(x - 2)^2 + (y + 1)^2 = 2

Center: (2,−1)(2, -1)

Step 2: Find slope of radius to point (1,−2)(1, -2) mradius=−2−(−1)1−2=−1−1=1m_{radius} = \frac{-2 - (-1)}{1 - 2} = \frac{-1}{-1} = 1

Step 3: Find slope of tangent Tangent is perpendicular to radius: mtangent=−1mradius=−11=−1m_{tangent} = -\frac{1}{m_{radius}} = -\frac{1}{1} = -1

Step 4: Equation of tangent at (1,−2)(1, -2) y−(−2)=−1(x−1)y - (-2) = -1(x - 1) y+2=−x+1y + 2 = -x + 1 x+y+1=0x + y + 1 = 0

Step 5: Equation of normal at (1,−2)(1, -2) Normal has slope mradius=1m_{radius} = 1: y−(−2)=1(x−1)y - (-2) = 1(x - 1) y+2=x−1y + 2 = x - 1 x−y−3=0x - y - 3 = 0

Table: Line Equations

Line Equation
Tangent x+y+1=0x + y + 1 = 0
Normal x−y−3=0x - y - 3 = 0

Mathematics Formula Cheat Sheet for Winter 2022 Exams

Determinants

  • 2×2 Matrix: ∣abcd∣=ad−bc\begin{vmatrix} a & b \\ c & d \end{vmatrix} = ad - bc
  • 3×3 Matrix: Expand along row/column with most zeros
  • Properties: If any row/column has all zeros, determinant = 0

Functions

  • Basic evaluation: f(1)=f(1) = substitute x=1x = 1 in f(x)f(x)
  • Tangent function properties:
    • f(x+y)=f(x)+f(y)1−f(x)f(y)f(x+y) = \frac{f(x) + f(y)}{1 - f(x)f(y)} when f(x)=tan⁡xf(x) = \tan x
    • f(2x)=2f(x)1−[f(x)]2f(2x) = \frac{2f(x)}{1 - [f(x)]^2} when f(x)=tan⁡xf(x) = \tan x

Logarithms

  • Basic properties:
    • log⁡1=0\log 1 = 0
    • log⁡x+log⁡(1x)=0\log x + \log(\frac{1}{x}) = 0
    • 1log⁡ab=log⁡ba\frac{1}{\log_a b} = \log_b a (Change of base)
  • Product rule: log⁡a+log⁡b=log⁡(ab)\log a + \log b = \log(ab)

Trigonometry

Angle Conversions

  • 120°=2π3120° = \frac{2\pi}{3} radians
  • General: degrees × π180\frac{\pi}{180} = radians

Inverse Functions

  • sin⁡−1(sin⁡θ)=θ\sin^{-1}(\sin \theta) = \theta if θ∈[−π2,π2]\theta \in [-\frac{\pi}{2}, \frac{\pi}{2}]
  • tan⁡−1a+tan⁡−1b=tan⁡−1(a+b1−ab)\tan^{-1} a + \tan^{-1} b = \tan^{-1}(\frac{a+b}{1-ab}) when ab<1ab < 1

Periods

  • sin⁡x\sin x, cos⁡x\cos x: period = 2π2\pi
  • tan⁡x\tan x: period = π\pi

Triple Angle Formulas

  • sin⁡3A=3sin⁡A−4sin⁡3A\sin 3A = 3\sin A - 4\sin^3 A
  • cos⁡3A=4cos⁡3A−3cos⁡A\cos 3A = 4\cos^3 A - 3\cos A

Allied Angles

  • sin⁡(θ+π)=−sin⁡θ\sin(\theta + \pi) = -\sin \theta
  • cos⁡(θ+2π)=cos⁡θ\cos(\theta + 2\pi) = \cos \theta
  • tan⁡(π2+θ)=−cot⁡θ\tan(\frac{\pi}{2} + \theta) = -\cot \theta

Vectors

  • Magnitude: ∣a⃗∣=a12+a22+a32|\vec{a}| = \sqrt{a_1^2 + a_2^2 + a_3^2}
  • Unit vector dot product: i^⋅i^=1\hat{i} \cdot \hat{i} = 1
  • Dot Product: a⃗⋅b⃗=a1b1+a2b2+a3b3\vec{a} \cdot \vec{b} = a_1b_1 + a_2b_2 + a_3b_3
  • Cross Product: a⃗×b⃗=∣i^j^k^a1a2a3b1b2b3∣\vec{a} \times \vec{b} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ a_1 & a_2 & a_3 \\ b_1 & b_2 & b_3 \end{vmatrix}
  • Perpendicularity: a⃗⊥b⃗\vec{a} \perp \vec{b} iff a⃗⋅b⃗=0\vec{a} \cdot \vec{b} = 0
  • Work done: W=F⃗⋅d⃗W = \vec{F} \cdot \vec{d}

Coordinate Geometry

Lines

  • Slope of vertical line: Undefined
  • Point-slope form: y−y1=m(x−x1)y - y_1 = m(x - x_1)
  • Parallel lines: Same slope
  • Angle between lines: tan⁡θ=∣m1−m21+m1m2∣\tan \theta = \left|\frac{m_1 - m_2}{1 + m_1m_2}\right|

Circles

  • Standard form: (x−h)2+(y−k)2=r2(x - h)^2 + (y - k)^2 = r^2
  • Center: (h,k)(h, k), Radius: rr
  • Tangent-radius relationship: Tangent ⊥ radius at point of contact

Limits

  • Standard limits:

    • lim⁡x→axn−anx−a=nan−1\lim_{x \to a} \frac{x^n - a^n}{x - a} = na^{n-1}
    • lim⁡n→0(1+n)1n=e\lim_{n \to 0} (1 + n)^{\frac{1}{n}} = e
    • lim⁡x→0sin⁡axbx=ab\lim_{x \to 0} \frac{\sin ax}{bx} = \frac{a}{b}
    • lim⁡x→0eax−1x=a\lim_{x \to 0} \frac{e^{ax} - 1}{x} = a
    • lim⁡x→∞(1+ax)x=ea\lim_{x \to \infty} (1 + \frac{a}{x})^x = e^a
  • L'Hôpital's Rule: For 00\frac{0}{0} or ∞∞\frac{\infty}{\infty} forms

  • Rational functions: Divide by highest power for x→∞x \to \infty

Series Formulas

  • 1+2+3+...+n=n(n+1)21 + 2 + 3 + ... + n = \frac{n(n+1)}{2}

Problem-Solving Strategies

For Determinant Problems

  1. Look for rows/columns with zeros
  2. Expand along the row/column with most zeros
  3. Factor common terms before expanding

For Function Composition

  1. Substitute inner function into outer function
  2. Simplify step by step
  3. Check domain restrictions

For Trigonometric Identities

  1. Use compound angle formulas
  2. Look for opportunities to use allied angles
  3. Convert everything to same trigonometric ratios

For Vector Problems

  1. Write in component form
  2. Use dot product for perpendicularity checks
  3. Use cross product for perpendicular vectors

For Limit Problems

  1. Try direct substitution first
  2. Factor and cancel for indeterminate forms
  3. Use standard limit formulas
  4. For exponential limits, use logarithms

For Circle Problems

  1. Complete the square to find center and radius
  2. Use slope relationships for tangent and normal
  3. Remember: tangent slope × radius slope = -1

Common Mistakes to Avoid

  1. Sign errors in determinant expansion
  2. Forgetting that vertical lines have undefined slope
  3. Not checking if point lies on circle before finding tangent
  4. Mixing up parallel (same slope) vs perpendicular (negative reciprocal slopes)
  5. Not simplifying trigonometric expressions fully
  6. Forgetting to rationalize in limit problems

Quick Reference Values

  • tan⁡30°=13\tan 30° = \frac{1}{\sqrt{3}}, tan⁡60°=3\tan 60° = \sqrt{3}, tan⁡45°=1\tan 45° = 1
  • e≈2.718e \approx 2.718
  • 3≈1.732\sqrt{3} \approx 1.732

Exam Success Tips

  • Show all steps clearly in calculations
  • Check answers by substitution when possible
  • Use proper notation throughout
  • Draw diagrams for vector and geometry problems
  • Manage time effectively across questions

Best of luck with your Winter 2022 Mathematics exam! 🎯

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