The probability density function of a continuous random variable \(X\) is given by
\(f(x)=\begin{cases}
\dfrac{x}{12} & 1 \leq x \leq 5 \\
\ \\
0 & \text {otherwise }
\end{cases}\)
Find \(P(X < 3)\) (2 marks)
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The probability density function of a continuous random variable \(X\) is given by
\(f(x)=\begin{cases}
\dfrac{x}{12} & 1 \leq x \leq 5 \\
\ \\
0 & \text {otherwise }
\end{cases}\)
Find \(P(X < 3)\) (2 marks)
\(\dfrac{1}{3}\)
\(\begin{aligned}
P(X & <3)\\
& =\int_1^3 \dfrac{1}{12} x d x \\
& =\dfrac{1}{12}\left[\frac{1}{2} x^2\right]_1^3 \\
& =\dfrac{1}{24}\left[3^2-1^2\right] \\
& =\dfrac{1}{3}
\end{aligned}\)
A continuous random variable, \(X\), has a probability density function given by
\(f(x)= \begin{cases}\dfrac{1}{5}\,e^{-\frac{x}{5}} & x \geq 0 \\
\ \\
0 & x<0
\end{cases}\)
The median of \(X\) is \(m\).
Determine the value of \(m\). (3 marks)
\(-5 \log _e\left(\dfrac{1}{2}\right)\) or \(5 \log _e(2)\) or \(\log _e 32\)
\(\begin{aligned} \dfrac{1}{5} \int_0^m e^{-\frac{x}{5}} d x & =\dfrac{1}{2} \\
\dfrac{1}{5} \times(-5)\left[e^{-\frac{x}{5}}\right]_0^m & =\dfrac{1}{2} \\
{\left[-e^{-\frac{x}{5}}\right]_0^m } & =\dfrac{1}{2} \\
-e^{-\frac{m}{5}}+1 & =\frac{1}{2} \\ e^{-\frac{m}{5}} & =\dfrac{1}{2} \\
-\frac{m}{5} & =\log _e\left(\dfrac{1}{2}\right)
\end{aligned}\)
\(\therefore m=-5 \log _e\left(\dfrac{1}{2}\right)\) (or \(5 \log _e(2)\), or \(\log _e 32\) )
The probability density function \(f(x)\) of a random variable \(X\) is given by
\(f(x)=\begin{cases}
\dfrac{x+1}{12} & 0 \leq x \leq 4 \\
\ \\
0 & \text{otherwise }
\end{cases}\)
Find the value of \(b\) such that \(P(X \leq b)=\dfrac{5}{8}\). (3 marks)
\(3\)
\(\begin{aligned}
\dfrac{1}{12} \int_0^b(x+1) d x & =\dfrac{5}{8} \\
{\left[\dfrac{1}{2} x^2+x\right]_0^b } & =\dfrac{15}{2} \\
\dfrac{1}{2} b^2+b & =\dfrac{15}{2} \\
b^2+2 b-15 & =0 \\ (b+5)(b-3) & =0
\end{aligned}\)
\(\therefore b=3 \quad(0 \leq b \leq 4)\)
The continuous random variable `X` has a distribution with probability density function given by
`f(x) = {(ax(5 - x), \ text(if)\ \ 0 <= x <= 5), (0,\ text (if)\ \ x < 0\ \ text(or if)\ \ x > 5):}`
where `a` is a positive constant.
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a. | `text(Total Area under curve)` | `= 1` |
`a int_0^5 (5x – x^2)\ dx` | `= 1` | |
`a [5/2 x^2 – 1/3 x^3]_0^5` | `= 1` | |
`a [(125/2 – 125/3) – (0)]` | `= 1` | |
`125/6 a` | `= 1` | |
`:. a` | `= 6/125` |
b. `P(X < 3) = int_0^3 ax(5 – x)\ dx`
The function `f(x)` is a probability density function of a continuous random variable with the rule
`f(x) = {(ae^x, 0 <= x <= 1), (ae, 1 < x <= 2), (\ 0, text(otherwise)):}`
The value of `a` is
A. `1`
B. `1/e`
C. `1/(2e)`
D. `1/(2e - 1)`
`D`
`text(Total area) = 1`
`int_0^1 ae^x\ dx + int_1^2 ae\ dx` | `= 1` |
`[ae^x]_0^1 + [ae*x]_1^2` | `=1` |
`[ae-a] + [2ae-ae]` | `=1` |
`2ae-a` | `=1` |
`a(2e-1)` | `=1` |
`:. a` | `= 1/(2e – 1)` |
`=> D`
If a continuous random variable \(X\) has probability density function
\(f(x)=
\begin{cases}
\dfrac{x}{2} & \text{if } \quad 0 \leq x \leq 2 \\
\ \\
0 & \text {otherwise }
\end{cases}\)
Find the exact value of \(p\) such that \(P(X>p) = 0.4\). (3 marks)
\(\dfrac{2 \sqrt{15}}{5}\)
\(\displaystyle \int_p^2 \dfrac{x}{2} d x=0.4\)
\(\begin{aligned} {\left[\dfrac{x^2}{4}\right]_p^2 } & =\dfrac{2}{5} \\
1-\dfrac{p^2}{4} & =\dfrac{2}{5} \\
\dfrac{p^2}{4} & =\dfrac{3}{5} \\ p^2 & =\dfrac{12}{5} \\
\therefore p & =\dfrac{2 \sqrt{3}}{\sqrt{5}} \\
& =\dfrac{2 \sqrt{15}}{5} \quad(0 \leq p \leq 2)
\end{aligned}\)
One bag contains red and green balls.
Kalyn randomly chooses one ball from the bag. Without replacement, he then chooses a second ball from the bag.
Complete the tree diagram below and then draw a probability distribution table for the number of red balls that could be drawn out of the bag. (3 marks)
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Evaluate `p` and `q` in the discrete probability distribution table below, given that `E(X) = 3`. (3 marks)
\begin{array} {|c|c|c|c|c|}
\hline
\rule{0pt}{2.5ex} x \rule[-1ex]{0pt}{0pt} & \ \ \ 1\ \ \ & \ \ \ 2\ \ \ & \ \ \ 3\ \ \ & \ \ \ 4\ \ \ \\
\hline
\rule{0pt}{2.5ex} P(X=x) \rule[-1ex]{0pt}{0pt} & p & q & 0.2 & 0.4 \\
\hline
\end{array}
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`text(See Worked Solutions)`
`p + q + 0.2 + 0.4` | `= 1` |
`p + q` | `= 0.4\ \ …\ (1)` |
`text(Given)\ \ E(X) = 3,`
`p + 2q + 0.6 + 1.6` | `= 3` |
`p + 2q` | `= 0.8\ \ …\ (2)` |
`text{Subtract: (2) – (1)}`
`q` | `= 0.4` |
`:.p` | `= 0` |
Prove that
`(1 - sin^2 x cos^2 x)/(sin^2 x) = cot^2 x + sin^2 x`. (2 marks)
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`text(See Worked Solutions)`
`text(RHS)` | `= (cos^2 x)/(sin^2 x) + sin^2 x` |
`= (cos^2 x + sin^4 x)/(sin^2 x)` | |
`= (cos^2 x + sin^2 x(1 – cos^2 x))/(sin^2 x)` | |
`= (cos^2 x + sin^2 x – sin^2 x cos^2 x)/(sin^2 x)` | |
`= (1 – sin^2 x cos^2 x)/(sin^2 x)` | |
`= \ text(LHS)` |
Sammy visits a giant Ferris wheel. Sammy enters a capsule on the Ferris wheel from a platform above the ground. The Ferris wheel is rotating anticlockwise. The capsule is attached to the Ferris wheel at point `P`. The height of `P` above the ground, `h`, is modelled by `h(t) = 65 - 55cos((pit)/15)`, where `t` is the time in minutes after Sammy enters the capsule and `h` is measured in metres.
Sammy exits the capsule after one complete rotation of the Ferris wheel.
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i. | `h_text(min)` | `= 65 – 55` | `h_text(max)` | `= 65 + 55` |
`= 10\ text(m)` | `= 120\ text(m)` |
ii. `text(Period) = (2pi)/(pi/15) = 30\ text(min)`
iii. | `h′(t)` | `=65 – 55cos((pit)/15)` |
`h′(t)` | `=pi/15 xx 55sin(pi/15 t)` | |
`= (11pi)/3\ sin(pi/15 t)` | ||
`text(S)text(ince)\ \ sin(pi/15 t)_text(max) = sin (pi/2),`
`:. h′(t)_text(max)\ \ text(occurs when)`
`(pi t)/15` | `=pi/2` | |
`:. t` | `=pi/2 xx 15/pi` | |
`=15/2\ text(minutes)\ \ (0<=t<=30)` |
Find the centre and radius of the circle with the equation
`x^2-12x + y^2 + 2y-12 = 0` (2 marks)
`text(Centre)\ (6, −1)`
`text(Radius = 7)`
`x^2-12x + y^2 + 2y-12` | `= 0` |
`(x-6)^2 + (y + 1)^2-36-1-12` | `= 0` |
`(x-6)^2 + (y + 1)^2` | `= 49` |
`:.\ text(Centre)\ (6, −1)`
`:.\ text(Radius = 7)`
Find the domain and range of `f(g(x))` given
`f(x) = 2x^2 - 8x` and `g(x) = x + 2`. (2 marks)
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`text(Domain: all)\ x`
`text(Range:)\ −8<=y< ∞`
`f(g(x))` | `= 2(x + 2)^2 – 8(x + 2)` |
`= 2(x^2 + 4x + 4) – 8x – 16` | |
`= 2x^2 + 8x + 8 – 8x – 16` | |
`= 2(x^2 – 4)` |
`:. text(Domain: all)\ x`
`:. text(Range:)\ −8<=y< ∞`
Given `f(x) = sqrtx` and `g(x) = 25 - x^2`
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`text(Range:)\ 0<=y<= 5`
i. | `g(f(x))` | `= 25 – (f(x))^2` |
`= 25 – (sqrtx)^2` | ||
`= 25 – x` |
ii. | `f(g(x))` | `= sqrt(g(x))` |
`= sqrt(25 – x^2)` |
`:.\ text(Domain:)\ −5<= x <= 5`
`:.\ text(Range:)\ 0<=y<= 5`
Let `f(x) = sin((2pix)/3)`.
Solve the equation `sin((2pix)/3) = -sqrt3/2` for `0<=x<=3` (2 marks)
`x = 2, 5/2`
`sin((2pix)/3) = -sqrt3/2`
`=>\ text(Base angle)\ = pi/3`
`(2 pi x)/3` | `=(4pi)/3, (5pi)/3, (10pi)/3, …` |
`:.x` | `=2 or 5/2, \ \ \ (0<=x<=3)` |
On any given day, the depth of water in a river is modelled by the function
`h(t) = 14 + 8sin((pit)/12),\ \ 0 <= t <= 24`
where `h` is the depth of water, in metres, and `t` is the time, in hours, after 6 am.
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i. `h_(text(min))\ text(occurs when)\ \ sin((pit)/12)=-1`
`:. h_(text(min))` | `= 14 – 8` |
`= 6\ text(m)` |
ii. | `14 + 8sin(pi/12t)` | `= 10` |
`sin(pi/12t)` | `= – 1/2` |
`text(Solve in general:)`
`pi/12t` | `=(7pi)/6 + 2pi n\ \ \ \ text(or)\ \ \ ` | `pi/12t` | `= (11t)/6 + 2pi n,` |
`t` | `= 14 + 24n` | `t` | `=22 + 24n` |
`text(Substitute integer values for)\ n,`
`:. t = 14quadtext(or)quad22,\ \ \ (0<=t<=24)`
Solve `2cos(2x) = −sqrt3` for `x`, where `0 <= x <= pi`. (2 marks)
`x = (5pi)/12, (7pi)/12`
`cos(2x)` | `= – sqrt3/2` |
`2x` | `= (5pi)/6, 2pi – (5pi)/6, 2pi+(5pi)/6` |
`=(5pi)/6, (7pi)/6, (17pi)/6,\ …` | |
`:. x` | `=(5pi)/12, (7pi)/12\ \ \ (0 <= x <= pi)` |
Solve the equation `cos((3x)/2) = 1/2` for `−pi/2<=x<=pi/2`. (2 marks)
`x = ± (2pi)/9`
`cos((3x)/2) = 1/2`
`=>\ text(Base angle)\ =pi/3`
`(3x)/2` | `= (-pi)/3, pi/3, (5pi)/3, …` |
`:. x` | `=(-2pi)/9, (2pi)/9, (10pi)/9` |
`= (-2pi)/9, (2pi)/9\ \ \ (−pi/2<=x<=pi/2)` |
Solve the equation `sin (x/2) = -1/2` for `2 pi<=x<= 4 pi` (2 marks)
`x = (7 pi)/3, (11 pi)/3`
`x/2` | `=pi/6 + pi, 2pi – pi/6, 2pi + (pi/6 +pi), …` |
`=(7pi)/6, (11pi)/6, (19pi)/6, …` | |
`:. x` | `=(7pi)/3, (11pi)/3, (19pi)/3, …` |
`text(Given)\ \ \2 pi<=x<= 4 pi`
`:. x = (7 pi)/3, (11 pi)/3`
Solve the equation
`sin (2x + pi/3) = 1/2\ \ text(for)\ \ 0<= x <=pi` (2 marks)
`x = pi/4, (11 pi)/12`
`sin (2x + pi/3) = 1/2`
`=>\ text(Base angle is)\ \ pi/6`
`(2x + pi/3)` | `= pi/6, (5pi)/6, (13pi)/6, (17pi)/6, …` |
`2x` | `= – pi/6, pi/2, (11pi)/6, (15pi)/6, …` |
`x` | `= – pi/12, pi/4, (11pi)/12, (15pi)/12, …` |
`:. x = pi/4, (11 pi)/12\ \ (0<=x<=pi)`
State the range and period of the function
`h(x) = 4 + 3 cos ((pi x)/2).` (2 marks)
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`text(Range:)\ \ 1<=y<= 7`
`text(Period) = 4`
`-1` | `<= cos ((pi x)/2)<=1` | |
`-3` | `<=3cos ((pi x)/2)<=3` | |
`1` | `<= 4+ 3cos ((pi x)/2)<=7` |
`:.\ text(Range:)\ \ 1<=y<= 7`
`text(Period) = (2pi)/n = (2 pi)/(pi/2) = 4`
Solve the equation `sqrt 3 sin x = cos x` for `– pi<=x<= pi`. (2 marks)
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`x = pi/6,\ \ \ – (5 pi)/6`
`text(Divide both sides by)\ \ cos x :`
`sqrt 3 sin x` | `=cos x` |
`sqrt 3 tan x` | `= 1` |
`tan x` | `= 1/sqrt 3` |
`=>\ text(Base angle)\ = pi/6` |
`:. x = pi/6\ \ text(or)\ – (5 pi)/6,\ \ \ (– pi <=x<= pi)`
The population of wombats in a particular location varies according to the rule `n(t) = 1200 + 400 cos ((pi t)/3)`, where `n` is the number of wombats and `t` is the number of months after 1 March 2018.
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i. `text(Period) = (2pi)/n = (2pi)/(pi/3) = 6\ text(months)`
`text(A)text(mplitude) = 400`
ii. `text(Max:)\ 1200 + 400 = 1600\ text(wombats)`
`text(Min:)\ 1200 – 400 = 800\ text(wombats)`
iii. | `n(10)` | `=1200 + 400 cos ((10 pi)/3)` |
`=1200 + 400 cos ((2 pi)/3)` | ||
`=1200-400 xx 1/2` | ||
`= 1000\ text(wombats)` |
iv. `text(Find)\ \ t\ \ text(when)\ \ n(t)=1000`
`1000` | `=1200 + 400 cos((pit)/3)` | |
`cos((pit)/3)` | `=- 1/2` | |
`(pit)/3` | `=(2pi)/3, (4pi)/3, (8pi)/3, (10pi)/3, … ` | |
`t` | `=2,4,8,10` |
`text(S)text(ince)\ \ n(0)=1600,`
`=> n(t)\ \ text(drops below 1000 between)\ \ t=2\ \ text(and)\ \ t=4,`
`text(and between)\ \ t=8\ \ text(and)\ \ t=10.`
`:.\ text(Fraction)` | `= (2 + 2)/12` |
`= 1/3\ \ text(year)` |
Let `f(x) = 2cos(x) + 1` for `0<=x<=2pi`.
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The graph shown could have equation
`=> B`
`text{Amplitude = 2 (range from – 1 to 3)}`
`text{Graph centre line (median):}\ \ y= 1`
`:.\ text(Eliminate)\ \ C\ \ text(and)\ \ D.`
`text(Period) = (2pi)/3 – pi/6 = pi/2\ \ text{(from graph)}`
`text(Consider option)\ B,`
`text(Period)= (2pi)/n= (2pi)/4 = pi/2`
`=> B`
The function with equation `f(x) = 4 tan (x/3)` has period
`D`
`text(Period) ` | `=pi/n` |
`= pi/(1/3)` | |
`= 3 pi` |
`=> D`
The UV index, `y`, for a summer day in Newcastle East is illustrated in the graph below, where `t` is the number of hours after 6 am.
The graph is most likely to be the graph of
`B`
`text{Centre line (median):} \ y = 5`
`text(Amplitude) = 5`
`text(Period:)\ \ 14` | `= (2 pi)/n` |
`n` | `= pi/7` |
`:.\ text(Graph:)\ \ y = 5 – 5 cos ((pi t)/7)`
`=> B`
A section of the graph of `f(x)` is shown below.
The equation of `f(x)` could be
`C`
`text(Period) = pi/2`
`=>\ text(must be)\ C\ text(or)\ D`
`text(Shift)\ \ y = tan(x)\ \ text(right)\ \ pi/4.`
`=> C`
Francis is buying a fridge. The energy usage of his two choices are below:
Fridge 1 (5 star rating): 227 kWh per year
Fridge 2 (2 star rating): 492 kWh per year
Each fridge has an expected life of 8 years.
If electricity costs 32.4 cents per kWh, how much will Francis save in electricity over the expected life of the more energy efficient fridge, to the nearest dollar? (2 marks)
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`$687`
`text(Energy cost of fridge 1)`
`= 227 xx 0.324 xx 8`
`= $588.38`
`text(Energy cost of fridge 2)`
`= 492 xx 0.324 xx 8`
`= $1275.26`
`:.\ text(Energy saving)` | `= 1275.26 – 588.38` |
`= 686.88` | |
`= $687` |
A potting mix is made up of two ingredients, potting soil and manure, in the ratio 5:2.
21 kilograms of potting mix are used to fertilise the rectangular vegetable garden pictured below.
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i. `text(Potting mix: 21 kg ⇒ 21, 000 grams)`
`text(Area of garden)` | `= 20 xx 7` | |
`= 140\ text(m²)` |
`:.\ text(Rate)` | `= (21\ 000)/140` |
`= 150\ text(g/m²)` |
ii. `text(Ratio 5 : 2)\ \ =>\ \ 5/7 : 2/7`
`:.\ text(Amount of manure)` | `= 2/7 xx 21` |
`= 6\ text(kg)` |
The network diagram below flows from the source (S) to sink (T).
Which of the edges is not at maximum capacity?
`=>\ text(C)`
A network diagram is drawn below.
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i. |
`text(Maximum flow)` | `=\ text(minimum cut)` |
`= 8 + 8 + 7 + 5` | |
`= 28` |
ii. |
|
Bianca is designing a project for producing an advertising brochure. It involves activities A-M.
The network below shows these activities and their completion time in hours.
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i. `text(Scanning forwards and backwards)`
`text{EST (activity}\ J) = 11\ text(hours)`
ii. | `text{LST (activity}\ H)` | `=\ text{LST}\ (H)-text(weight)\ (H)` |
`= 20-2` | ||
`=18\ text(hours)` |
iii. | `text{Float time}\ (I)` | `=\ text(LST)\ (I)-text(EST)\ (I)` |
`=12-10` | ||
`= 2\ text(hours)` |
iv. `text(Critical Path is)\ CGJLM`
`:.\ text(Minimum time)` | `= 2 + 9 + 6 + 7 + 10` |
`= 34\ text(hours)` |
At her favourite fun park, Katherine’s first activity is to slide down a 10 m long straight slide. She starts from rest at the top and accelerates at a constant rate, until she reaches the end of the slide with a velocity of `6\ text(ms)^(-1)`.
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When at the top of the slide, which is 6 m above the ground, Katherine throws a chocolate vertically upwards. The chocolate travels up and then descends past the top of the slide to land on the ground below. Assume that the chocolate is subject only to gravitational acceleration and that air resistance is negligible.
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At what velocity would the chocolate need to be propelled upwards, if Katherine were to immediately slide down the slide and run to reach the chocolate just as it hits the ground?
Give your answer in `text(ms)^(-1)`, correct to one decimal place. (2 marks)
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Katherine’s next activity is to ride a mini speedboat. To stop at the correct boat dock, she needs to stop the engine and allow the boat to be slowed by air and water resistance.
At time `t` seconds after the engine has been stopped, the acceleration of the boat, `a\ text(ms)^(-2)`, is related to its velocity, `v\ text(ms)^(-1)`, by
`a = -1/10 sqrt(196-v^2)`.
Katherine stops the engine when the speedboat is travelling at `7\ text(m/s)`.
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a. `u = 0, quad v = 6, quad s = 10`
`text(Solve for)\ \ t:\ \ \ ((u + v)/2)t` | `= s` |
`((0 + 6)/2)t` | `= 10` |
`t` | `= 10/3\ text(s)` |
b. `u = 10, quad a = -9.8, quad s = -6`
`text(Solve for)\ \ t:`
`s` | `= ut + 1/2 at^2` |
`-6` | `= 10t-4.9 t^2` |
`:. t` | `~~2.5\ text(s)\ \ \ text{(by CAS)}` |
c. `text(Time of chocolate in air)`
`= 10/3 + 4`
`=22/3`
`text(Solve for)\ \ u:`
`-6` | `= 22/3 u -4.9(22/3)^2` |
`:. u` | `~~35.1\ text(m s)^(−1)\ \ \ text{(by CAS)}` |
d.i. | `(dv)/(dt)` | `= -1/10 sqrt(196-v^2)` |
`(dt)/(dv)` | `= (-10)/sqrt(196-v^2)` | |
`t` | `= int(-10)/sqrt(196-v^2)\ dv` | |
`-t/10` | `= int 1/sqrt(14^2-v^2) dv` | |
`-t/10` | `= sin^(-1)(v/14) + c` |
`text(When)\ \ t = 0, v = 7`
`=> c=-sin^(-1)(1/2) = -pi/6`
`-t/10` | `=sin^(-1)(v/14)-pi/6` | |
`sin^(-1) (v/14)` | `= pi/6-t/10` | |
`:. v` | `=14sin(pi/6-t/10)` |
d.ii. `text(Find)\ \ t\ \ text(when)\ \ v=0:`
`-t/10` | `=sin^(-1)(0)-pi/6` | |
`t` | `= -10 sin^(-1)(0) + (10 pi)/6` | |
`= (5 pi)/3\ text(s)` |
d.iii. `v = 14sin(pi/6-t/10)`
`(dx)/(dt)` | `=14sin(pi/6-t/10)` |
`x` | `= int_0^((5pi)/3)14sin(pi/6-t/10)\ dt` |
`~~ 18.8\ text(m)\ \ \ text{(by CAS)}` |
The position vector of the International Space Station `text{(S)}`, when visible above the horizon from a radar tracking location `text{(O)}` on the surface of Earth, is modelled by
`underset ~r(t) = 6800 sin(pi(1.3t-0.1))underset~i + (6800 cos(pi(1.3t-0.1))-6400)underset ~j`,
for `t in [0, 0.154]`,
where `underset ~i` is a unit vector relative to `text(O)` as shown and `underset ~j` is a unit vector vertically up from point `text(O)`. Time `t` is measured in hours and displacement components are measured in kilometres.
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a. `text(At)\ \ P,\ \ x(t)=0`
`text{Solve (by CAS):}\ \ 6800 sin (pi(1.3t-0.1))` | `= 0` |
`=> t=0.076923…`
`:. h` | `= 6800 cos (pi (1.3(0.076923)-0.1))-6400` |
`= 400` |
b. | `underset ~(dot r) (t)` | `= 8840pi cos (pi(1.3t-0.1)) underset ~i-8840pi sin (pi(1.3t-0.1)) underset ~j` |
`underset ~(ddot r) (t)` | `= -11\ 492 pi^2 sin (pi(1.3t-0.1))underset ~i-11\ 492 pi^2 cos (pi(1.3t-0.1)) underset ~j` |
`text(Let)\ \ u=pi(1.3t-0.1),`
`underset ~(ddot r) (t) ⋅ underset ~(dot r) (t)` | `= -(8840)(11\492) pi^3 cos (u) sin (u) + (8840)(11\492) pi^3 cos(u)sin(u)`
|
`= 0` |
`:. underset ~(ddot r) (t) _|_ underset ~(dot r) (t)`
c. `text(Speed)\ = |\ dotr(t)\ |`
`|\ dotr(t)\ |` | `= sqrt((8840pi)^2 cos^2(pi(1.3t-0.1)) + (8840pi)^2 sin^2 (pi(1.3t-0.1)))` |
`= 8840 pi` | |
`~~ 27\ 772` |
d. | `x/6800` | `= sin(pi(1.3t-0.1))` |
`(6400 + y)/6800` | `= cos(pi (1.3t-0.1))` |
`text(Using)\ \ sin^2theta + cos^2theta = 1`
`x^2/6800^2 + (6400 + y)^2/6800^2` | `=1` | |
`x^2 + (y + 6400)^2` | `= 6800^2` |
e. `underset ~r(t) = 6800 sin(u)underset~i + (6800 cos(u)-6400)underset ~j`
`text(Find)\ \ t\ \ text(such that)\ \ |\ underset ~r(t)\ | = 1000:`
`6800^2sin^2(u) + (6800 cos(u) -6400)^2 = 1000^2,\ \ \ (u=pi(1.3t-0.1))`
`6800^2-2 xx 6400 xx 6800 cos(u) + 6400^2 = 1000^2`
`=>cos(pi(1.3t-0.1)) = 0.9903\ \ \ text{(by CAS)}`
`:. t=0.04 or 0.11`
A car accelerates from rest. Its speed after `T` seconds is `V\ text(ms)^(−1)`, where
`V = 17 tan^(−1)((pi T)/6), T >= 0`
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After accelerating to `25\text(ms)^(−1)`, the car stays at this speed for 120 seconds and then begins to decelerate while braking. The speed of the car `t` seconds after the brakes are first applied is `v\ text(ms)^(−1)` where
`(dv)/(dt) =-1/100 (145-2t),`
until the car comes to rest.
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Give your answer in metres correct to the nearest metre. (1 mark)
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`d_2 = 25 xx 120`
`d_3 = int_0^20 -1/100 [145 t-t^2] + 25\ dt`
a. `text(As)\ \ T->oo,\ \ tan^(-1)((piT)/6)->pi/2`
`:.underset (T->oo) (limV)` | `= (17 pi)/2` |
b. `(dV)/(dt)= (102 pi)/(36 + pi^2 T^2),\ \ \ text{(by CAS)}`
`text(When)\ \ T=10:`
`(dV)/(dt)` | `= (102 pi)/(36 + 100 pi^2)` |
`~~ 0.3` |
c. `text(Find)\ \ T\ \ text(when)\ \ V=25:`
`17 tan^(-1) ((pi T)/6)` | `=25 ` | |
`T` | `= 18.995\ \ \ text{(by CAS)}` | |
`~~ 19\ text(seconds)` |
d.i. | `v` | `= -1/100 int_0^t 145-2t\ dt` |
`v` | `= -1/100 [145 t-t^2] + c` |
`text(When)\ \ t=0, \ v=25:`
`=> c=25`
`:. v= -1/100 [145 t-t^2] + 25`
d.ii. `text(Find)\ \ t\ \ text(when)\ \ v=0:`
`-1/100[145t-t^2] + 25=0`
`:. t=20\ text(seconds)\ \ \ text{(by CAS)}`
e.i. `text(Stage 1: car travels from rest to 25 m/s)`
`d_1 = int_0^19 17 tan^(-1) ((pi T)/6)\ dT`
`text(Stage 2: car travels at 25 m/s for 120 seconds)`
`d_2` | `= 25 xx 120` |
`= 3000` |
`text(Stage 3: car decelerates for 20 seconds`
`d_3 = int_0^20 -1/100 [145 t-t^2] + 25\ dt`
e.ii. | `d_1` | `~~ 400.131` |
`d_2` | `= 3000` | |
`d_3` | `= 236.6` |
`text(Total distance)` | `= d_1 + d_2 + d_3` |
`~~ 3637\ text(m)` |
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`{z: text(Arg)(z_1) <= text(Arg)(z) <= text(Arg)(z_1^4)} ∩ {z: 1 <= |\ z\ | <= 2}, z ∈ C`. (2 marks)
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ii. `z_1^4 = text(cis) pi/3`
ii. `z_1^n = ±i\ text(for)\ k ∈ Z`
a. | `cos^2(pi/12) + sin^2(pi/12)` | `= 1` |
`sin^2(pi/12)` | `= 1-(sqrt 3 + 2)/4` | |
`= (2-sqrt 3)/4` |
`:. sin (pi/12) = sqrt(2-sqrt 3)/2,\ \ \ (sin (pi/12) > 0)`
b.i. | `z_1` | `= cos(pi/12) + i sin (pi/12)` |
`= text(cis)(pi/12)` |
b.ii. | `z_1^4` | `= 1^4 text(cis) ((4 pi)/12)` |
`= text(cis)(pi/3)` |
c. |
d. `text(Area of large sector)`
`=theta/(2pi) xx pi r^2`
`=(pi/3-pi/12)/(2pi) xx pi xx 2^2`
`=pi/2`
`text(Area of small sector)`
`=1/2 xx pi/4 xx 1`
`=pi/8`
`:.\ text(Area shaded)`
`= pi/2-pi/8`
`= (3 pi)/8`
e.i. | `z_1^n` | `= 1^n text(cis) ((n pi)/12)` |
`text(Re)(z_1^n)` | `= cos((n pi)/12) = 0` | |
`(n pi)/12` | `=cos^(-1)0 +2pik,\ \ \ k in ZZ` | |
`(n pi)/12` | `= pi/2 + k pi` | |
`n` | `= 6 + 12k,\ \ \ k in ZZ` |
e.ii. `text(When)\ \ n=(6 + 12k):`
`z_1^n` | `= 1^(6 + 12k) text(cis) (((6 + 12k)pi)/12), quad k in ZZ` | |
`= i xx sin (((6 + 12k)pi)/12)` | ||
`= i xx sin (pi/2 + k pi)` |
`text(If)\ \ k=0 or text(even,)\ \ z_1^n=i`
`text(If)\ \ k\ text(is odd,)\ \ z_1^n=-i`
`:. z_1^n = +-i,\ \ \ k in ZZ`
A 12 kg mass is suspended in equilibrium from a horizontal ceiling by two identical light strings. Each string makes an angle of 60° with the ceiling, as shown.
The magnitude, in newtons, of the tension in each string is equal to
A. `6 g`
B. `12 g`
C. `24 g`
D. `4 sqrt 3 g`
E. `8 sqrt 3 g`
`D`
If `underset ~u = 2 underset ~i - 2 underset ~j + underset ~k` and `underset ~v = 3 underset ~i - 6 underset ~j + 2 underset ~k`, the vector resolute of `underset ~v` in the direction of `underset ~u` is
A. `20/49(3 underset ~i - 6 underset ~j + 2 underset ~k)`
B. `20/3(2 underset ~i - 2underset ~j + underset ~k)`
C. `20/7(3 underset ~i - 6 underset ~j + 2 underset ~k)`
D. `20/9(2 underset ~i - 2 underset ~j + underset ~k)`
E. `1/9(−2 underset ~i + 2 underset ~j - underset ~k)`
`D`
`tildeu = 2tildei – 2tildej + tildek,qquadtildev = 3tildei – 6tilde j + 2tildek`
`|\ tildeu\ |` | `= sqrt(2^2 + (−2)^2 + 1^2)=3` |
`hatu` | `= = 1/3(2tildei – 2tildej + tildek)` |
`tildev*hatu\ \ (text(Scalar resolute of)\ tildev\ text(in the direction of)\ tildeu)`
`= (3tildei – 6tildej + 2tildek)* 1/3(2tildei – 2tildej + tildek)`
`= 20/3`
`(tildev*hatu)hatu\ \ (text(Vector resolute of)\ tildev\ text(in the direction of)\ tildeu)`
`= 20/3 xx 1/3(2tildei – 2tildej + tildek)`
`= 20/9(2tildei – 2tildej + tildek)`
`=> D`
A particle is acted on by two forces, one of 6 newtons acting due south, the other of 4 newtons acting in the direction N60° W.
The magnitude of the resultant force, in newtons, acting on the particle is
`B`
Using a suitable substitution, `int_0^(pi/3) sin^3 (x) cos^4 (x)\ dx` can be expressed in terms of `u` as
A. `int_0^(pi/3) (u^6 - u^4)\ du`
B. `int_1^(1/2) (u^6 - u^4)\ du`
C. `int_(1/2)^1 (u^6 - u^4)\ du`
D. `int_0^(sqrt3/2) (u^6 - u^4)\ du`
E. `int_0^(sqrt3/2) (u^4 - u^6)\ du`
`B`
`text(Let)\ \ u = cos(x)`
`(du)/(dx) = -sin(x)\ \ =>\ \ du=-sin(x)\ dx`
`sin^2(x)` | `= 1 – cos^2(x)` |
`= 1 – u^2` |
`text(When)\ \ x = 0, \ u = 1`
`text(When)\ \ x = pi/3, \ u = 1/2`
`int_0^(pi/3) sin^3 (x) cos^4 (x)\ dx`
`=-int_1^(1/2) (1 – u^2)u^4\ du`
`= int_1^(1/2) (u^6 – u^4)\ du`
`=> B`
If `(d^2y)/(dx^2) = x^2 - x` and `(dy)/(dx) = 0` at `x = 0`, then the graph of `y` will have
`E`
`(d^2y)/(dx^2)=x^2-x`
`(d^2y)/(dx^2)=0\ \ text(when)\ \ x=0 or 1`
`(dy)/(dx)` | ` = (x^3)/3 – (x^2)/2 + c` |
`= x^2(x/3 – 1/2) + c` |
`text(Given)\ \ (dy)/(dx) = 0\ \ text(when)\ \ x = 0\ \ =>\ \ c=0`
`(dy)/(dx) = 0\ \ text(when)\ \ x = 0 or 3/2`
`(d^2y)/(dx^2)|_(x = 3/2) = 3/4>0`
`:.\ text(Local minimum at)\ \ x = 3/2`
`text(At)\ \ x=0, dy/dx<0\ \ text(either side)`
`:.\ text(Stationary point of inflection at)\ x=0`
`text(At)\ \ x=1, \ dy/dx!=0, \ dy/dx<0\ \ text(either side)`
`:.\ text(Non-stationary point of inflection at)\ \ x = 1`
`=> E`
The diagram that best represents the direction field of the differential equation `(dy)/(dx) = xy` is
A. | B. | ||
C. | D. |
`A`
`(dy)/(dx) = xy`
`text(When)\ \ x=0 \ or\ y=0\ \ =>\ text(gradient = 0)`
`text(In 1st and 3rd quartile)\ \ =>\ \ text(gradients positive)`
`text(In 2nd and 4th quartile)\ \ =>\ \ text(gradients negative)`
`=> A`
Euler's formula is used to find `y_2`, where `(dy)/(dx) = cos(x),\ x_0 = 0, \ y_0 = 1` and `h = 0.1`.
The value of `y_2` correct to four decimal places is
A. 1.1000 and this is an underestimate of `y(0.2)`
B. 1.1995 and this is an overestimate of `y(0.2)`
C. 1.1995 and this is an underestimate of `y(0.2)`
D. 1.2975 and this is an underestimate of `y(0.2)`
E. 1.2975 and this is an overestimate of `y(0.2)`
`B`
`x_0 = 0,\ \ y_0 = 1,\ \ h=0.1`
`y_1` | `= y_0 + h* (dy)/(dx)|_{(0,1)}` |
`= 1 + 0.1 xx cos(0)` | |
`= 1.1` | |
`y_2` | `= 1.1 + 0.1 xx cos(0.1)` |
`~~ 1.1995` |
`text(S)text(ince)\ \ sin(x)\ \ text(is concave down in the region)\ \ x=0.2,`
`1.1995\ text(is an overestimate.)`
`=> B`
A particle moves in a straight line. At time `t` seconds, where `t >= 0`, its displacement `x` metres from the origin and its velocity `v` metres per second are such that `v = 25 + x^2`.
If `x = 5` initially, then `t` is equal to
`E`
`(dx)/(dt) = 25 + x^2`
`(dt)/(dx) = 1/(25 + x^2)`
`t` | `= int 1/(25 + x^2)\ dx` |
`= 1/5 int 5/(5^2 + x^2)\ dx` | |
`= 1/5 tan^(−1)(x/5) + c` |
`text(When)\ \ t=0,\ \ x=5:`
`0` | `= 1/5 tan^(−1)(5/5) +c` |
`c` | `= – pi/20` |
`:. t= 1/5 tan^(−1)(x/5) – pi/20`
`=> E`
A body moves in a straight line such that its velocity `v\ text(ms)^(-1)` is given by `v = 2sqrt(1 - x^2)`, where `x` metres is its displacement from the origin.
The acceleration of the body in `text(ms)^(-2)` is given by
`E`
`v = 2(sqrt(1 – x^2))`
`a` | `=v *(dv)/(dx)` | |
`= 2sqrt(1 – x^2) xx 2 xx (−2x) xx 1/(2sqrt(1 – x^2))` | ||
`= −(4x sqrt(1 – x^2))/sqrt( 1 – x^2)` | ||
`= −4x` |
`=> E`
The motion of a lift (elevator) in a shopping centre is given by the velocity-time graph below, where time `t` is in seconds, and the velocity of the lift is `v` metres per second. For `v > 0` the lift is moving upwards.
The graph shows that at the end of 30 seconds, the position of the lift is
A. 17.5 metres above its starting level.
B. 5 metres above its starting level.
C. at the same position as its starting level.
D. 5 metres below its starting level.
E. 17.5 metres below its starting level.
`A`
`text(Distance)` | `= text(Area of trap) – text(Area of triangle)` |
`= 1/2(5 + 15)3 – 1/2 xx 10 xx 2.5` | |
`= 17.5\ text(m)` |
`text{Net area is above the}\ xtext{-axis (lift is higher).}`
`=> A`
The amount of chemical `x` in a tank at time `t` is given by the differential equation `dx/dt = -10/(10 - t)` and when `t = 0`, `\ x_0 = 5`. Euler's method is used with a step size of 0.5 in the values of `t`.
The value of `x` correct to two decimal places when `t = 1` is found to be
A. 3.95
B. 3.97
C. 4.50
D. 5.50
E. 6.03
`B`
`x_1 ~~ x(0.5)` | `= 5 + 0.5 xx (−10/(10 – 0))` |
`= 5 – 0.5` | |
`= 4.5` |
`x_2 ~~ x(1)` | `= 4.5 + 0.5 xx (−10/(10 – 0.5))` |
`= 4.5 – 10/19` | |
`~~ 3.97` |
`=> B`
The differential equation which best represents the above direction field is
A. `(dy)/(dx) = (y - 2x)/(2y + x)`
B. `(dy)/(dx) = (2x - y)/(y - 2x)`
C. `(dy)/(dx) = (2y - x)/(y + 2x)`
D. `(dy)/(dx) = (y - 2x)/(2y - x)`
E. `(dy)/(dx) = (x - 2y)/(2y + x)`
`A`
`text(When)\ \ x=0\ \ => \ \ text(gradients are all positive)`
`text(Eliminate B and E.)`
`text(When)\ \ y=0\ \ => \ \ text(gradients are all negative)`
`text(Eliminate D.)`
`text(Option A will have zero gradient along)\ \ y=2x\ \ text{(correct)}`
`text(Option C will have zero gradient along)\ \ y=1/2 x\ \ text{(incorrect)}`
`=> A`
Using a suitable substitution, the definite integral `int_0^(pi/24)tan(2x)sec^2(2x)\ dx` is equivalent to
A. `1/2int_0^(pi/24)(u)\ du`
B. `2int_0^(pi/24)(u)\ du`
C. `int_0^(2 - sqrt3)(u)\ du`
D. `1/2int_0^(2 - sqrt3)(u)\ du`
E. `2int_0^(2 - sqrt3)(u)\ du`
`D`
`text(Let)\ \ u = tan(2x)`
`(du)/dx = 2 sec^2(2x)\ \ =>\ \ 1/2 du = sec^2(2x)\ dx`
`text(When)\ \ x=pi/24\ \ =>\ \ u=tan(pi/12)=2-sqrt3\ \ text{(by CAS)}`
`text(When)\ \ x=0\ \ =>\ \ u=0`
`:. int_0^(pi/24)tan(2x)sec^2(2x)\ dx`
`= 1/2int_0^(2 – sqrt3)(u)\ du`
`=> D`
If `f″(x) = 2e^xsin(x)`, `f′(0) = 0` and `f(0) = 0`, the `f(x)` equals
A. `−e^x(cos(x) + sin(x))`
B. `−e^x(cos(x) - sin(x)) + 1`
C. `−e^xcos(x)`
D. `x - e^xcos(x) + 1`
E. `x - e^xcos(x)`
`D`
`text(Consider:)\ \ f(0)=0,`
`=>\ text(Eliminate A, C and E.)`
`text(By CAS, B and D satisfy)\ \ f′(0) = 0.`
`text(By CAS, only D satisfies)\ \ f″(x) = 2e^x sin(x)`
`=> D`
The position of a particle at time `t` is given by `underset~r(t) = (sqrt(t - 2))underset~i + (2t)underset~j` for `t >= 2`.
The cartesian equation of the path of the particle is
A. `y = 2x^2 + 4`, | `x >= 2` |
B. `y = 2x^2 + 2`, | `x >= 2` |
C. `y = 2x^2 + 4`, | `x >= 0` |
D. `y = sqrt((x - 4)/2)`, | `x >= 4` |
E. `y = 2x^2 + 2`, | `x >= 0` |
`C`
`tilder(t) = (sqrt(t – 2)tildei + (2t)tildej)`
`x = sqrt(t – 2)`
`text(Given)\ \ t >= 2\ \ =>\ \ x >=0`
`y = 2t\ \ =>\ \ t = y/2`
`:. x` | `= sqrt(y/2 – 2)` |
`x^2` | `= y/2 – 2` |
`y/2` | `= x^2 + 2` |
`y` | `= 2x^2 + 4` |
`=> C`
Consider the three forces
`underset~F_1 = −sqrt3underset~j`, `underset~F_2 = underset~i + sqrt3underset~j` and `underset~F_3 = −1/2underset~i + sqrt3/2underset~j`.
The magnitude of the sum of these three forces is equal to
`E`
`underset~(F_1) + underset~(F_2) + underset~(F_3)` | `= (1 – 1/2)underset~i + (−sqrt3 + sqrt3 + sqrt3/2)underset~j` |
`= 1/2 underset~i + sqrt3/2underset~j` |
`|underset~(F_1) + underset~(F_2) + underset~(F_3)|` | `= sqrt((1/2)^2 + (sqrt3/2)^2)` |
`= |underset~(F_3)|` |
`=> E`
The diagram below shows a rhombus, spanned by the two vectors `underset~a` and `underset~b`.
It follows that
A. `underset~a.underset~b = 0`
B. `underset~a = underset~b`
C. `(underset~a + underset~b).(underset~a - underset~b) = 0`
D. `|\ underset~a + underset~b\ | = |\ underset~a - underset~b|`
E. `2underset~a + 2underset~b = underset~0`
`C`
`text(Consider A:)`
`text(If)\ \ underset~a · underset~b = 0\ \ =>\ \ underset~a ⊥ underset~b\ \ text{(incorrect)}`
`text(Consider B:)`
`underset~a != underset~b\ \ text{(incorrect)}`
`text(Consider C:)`
`underset~a + underset~b` | `= overset(->)(OC)` |
`underset~a – underset~b` | `= overset(->)(BA)` |
`overset(->)(OC) · overset(->)(BA)=0`
`text{The diagonals of a rhombus are perpendicular (correct)}`
`=> C`
In the complex plane, the circle with equation `|\ z - (2 + 3i)\ | = 1` is intersected exactly twice by the curve with equation
A. `|\ z - 3i\ | = 1`
B. `|\ z + 3\ | = |\ z - 3i\ |`
C. `|\ z - 3\ | = |\ z - 3i\ |`
D. `text(Im)(z) = 4`
E. `text(Re)(z) = 3`
`C`
The polynomial `P(z)` has real coefficients. Four of the roots of the equation `P(z) = 0` are `z = 0`, `z = 1 - 2i`, `z = 1 + 2i` and `z = 3i`.
The minimum number of roots that the equation `P(z) = 0` could have is
A. 4
B. 5
C. 6
D. 7
E. 8
`B`
`P(z) = 0\ text(has real coefficients,)`
`=>\ text(Conjugate root theorem applies)`
`z = −3i\ \ text(is also a root)`
`:.\ text(Minimum roots = 5)`
`=> B`
A certain complex number `z`, where `|\ z\ | > 1`, is represented by the point on the following argand diagram.
All axes below have the same scale as those in the diagram above.
The complex number `1/barz` is best represented by
`C`
`|z| > 1`
`|1/(barz)| < 1`
`1/(barz)` | `= 1/(x – iy) xx (x + iy)/(x + iy)` |
`= (x + iy)/(x^2 + y^2)` | |
`= z/(|z|^2)` |
`:.\ 1/barz\ \ text(has same argument as)\ z,\ text(smaller magnitude.)`
`=> C`
The region in the first quadrant enclosed by the curve `y = sin(x)`, the line `y = 0` and the line `x = pi/6` is rotated about the `x`-axis. Find the volume of the resulting solid of revolution. (3 marks) --- 8 WORK AREA LINES (style=lined) ---
`pi^2/12-(sqrt3 pi)/8\ \ text(u³)`
The velocity–time graph for the first 2 seconds of the motion of a particle that is moving in a straight line with respect to a fixed point is shown below.
The particle’s velocity `v` is measured in cm/s. Initially the particle is `x_0` cm from the fixed point.
The distance travelled by the particle in the first 2 seconds of its motion is given by
A. `int_0^2 v\ dt`
B. `int_0^2 v\ dt + x_0`
C. `int_1^2 v\ dt - int_0^1 v\ dt`
D. `|\ int_0^2 v\ dt\ |`
E. `int_1^2 v\ dt - int_0^1 v\ dt + x_0`
`C`
`text(Distance = Total area between curve and the axis)`
`d= int_1^2 v\ dt – int_0^1 v\ dt`
`=> C`
Consider the three vectors `underset ~a = underset ~i - underset ~j + 2underset ~k,\ underset ~b = underset ~i + 2 underset ~j + m underset ~k` and `underset ~c = underset ~i + underset ~j - underset ~k`, where `m in R.` --- 4 WORK AREA LINES (style=lined) --- --- 4 WORK AREA LINES (style=lined) --- --- 3 WORK AREA LINES (style=lined) --- --- 4 WORK AREA LINES (style=lined) ---
c.i. `3 underset ~c – underset ~a` `=3underset~i – underset~i + 3underset~j + underset~j -3underset~k – 2underset~k` `=2underset~i + 4underset~j-5underset~k` c.ii. `text(Linear dependence)\ \ =>\ \ 3underset~c – underset~a = t underset~b,\ \ t in RR` `2 tilde i + 4 tilde j – 5 tilde k= t (tilde i + 2 tilde j + m tilde k)` `=> t = 2 and tm = -5,` `:. m=-5/2`
a.
`|underset~b|`
`= sqrt(1^2 + 2^2 + m^2)`
`= 2sqrt3`
`1 + 4 + m^2`
`= 4 xx 3`
`m^2`
`= 7`
`m`
`= ±sqrt7`
b.
`underset~a * underset~b`
`= 1 xx 1 + (−1) xx 2 + 2 xx m`
`0`
`= 1 – 2 + 2m\ \ ( underset~a ⊥ underset~b)`
`2m`
`= 1`
`m`
`= 1/2`