A solid is formed by rotating the region bounded by the curve $y = x(x - 1)^2$ and the line $y = 0$ about the y-axis - HSC - SSCE Mathematics Extension 2 - Question 5 - 2006 - Paper 1
Question 5
A solid is formed by rotating the region bounded by the curve $y = x(x - 1)^2$ and the line $y = 0$ about the y-axis. Use the method of cylindrical shells to find th... show full transcript
Worked Solution & Example Answer:A solid is formed by rotating the region bounded by the curve $y = x(x - 1)^2$ and the line $y = 0$ about the y-axis - HSC - SSCE Mathematics Extension 2 - Question 5 - 2006 - Paper 1
Step 1
A solid is formed by rotating the region bounded by the curve $y = x(x - 1)^2$ and the line $y = 0$ about the y-axis. Use the method of cylindrical shells to find the volume of this solid.
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Answer
To find the volume of the solid, we apply the method of cylindrical shells:
The formula for the volume using cylindrical shells is given by:
V=2π∫abxf(x)dx
where f(x)=y=x(x−1)2 and the limits of integration are determined from the points where the curve intersects the line y=0.
We first find the x-intercepts of y=x(x−1)2:
Setting y=0, we find x=0 and x=1 (the points of intersection).
Thus, the volume is:
V=2π∫01x[x(x−1)2]dx=2π∫01(x3−2x2+x)dx
Now, calculating the integral:
=2π[4x4−32x3+2x2]01=2π(41−32+21)
Simplifying this expression will yield the volume.
Step 2
(b) (i) Show that $\cos(\alpha + \beta) + \cos(\alpha - \beta) = 2\cos \alpha \cos \beta$.
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To show this identity:
We can use the cosine angle addition formula:
cos(α+β)=cosαcosβ−sinαsinβcos(α−β)=cosαcosβ+sinαsinβ
By adding the two equations:
cos(α+β)+cos(α−β)=2cosαcosβ
This proves the identity as required.
Step 3
(b) (ii) Hence, or otherwise, solve the equation $\cos^4 + \cos 2\theta + \cos 3\theta + \cos 4\theta = 0$ for $0 \leq \theta \leq 2\pi$.
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To solve the equation:
From part (i), we know how to relate angles using cosines. We first apply the identities:
Rewrite cos2θ, cos3θ, and cos4θ using double angle formulas.
Substitute:
The equation simplifies to a polynomial which can be factored or solved numerically.
The roots can be found in the given interval by testing values or using numerical methods.
Step 4
(c) (i) Resolve the forces on P in the horizontal and vertical directions.
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Answer
To resolve the forces on particle P:
In the horizontal direction, the tension T1 provides a component:
T1sinα
This is the centripetal force due to the motion, equal to mω2r.
In the vertical direction, we balance the forces:
T1cosα+T2=mg
where T2 is the tension in the second string.
Step 5
(c) (ii) If $T_2=0$, find the value of $\omega$ in terms of $l$, $g$, and $\alpha$.
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To find ω under the condition that T2=0:
We start from the vertical force equation:
T1cosα=mg
Thus, we express T1:
T1=cosαmg
Using the horizontal component:
T1sinα=mω2l
Substituting for T1:
cosαmgsinα=mω2l
Simplifying and solving for ω, we get:
ω=lgtanα
Step 6
(d) (i) How many different recordings are possible?
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To find the number of different recordings:
For each of the four games, there are three potential outcomes (Win, Draw, Loss). Thus,
34=81 different outcomes are possible.
Step 7
(d) (ii) Calculate the probability of the result which is recorded as WDLD.
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To calculate the probability of the result WDLD:
The probability of each outcome is:
Win (W): 0.2
Draw (D): 0.6
Loss (L): 0.2
Thus, the probability of WDLD is:
P(WDLD)=P(W)⋅P(D)⋅P(L)⋅P(D)=0.2⋅0.6⋅0.2⋅0.6=0.0144.
Step 8
(d) (iii) What is the probability that the Home team scores more points than the Away team?
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To find this probability:
The scoring system gives:
1 point for a win, \frac{1}{2} point for a draw, and 0 points for a loss.
Considering all configurations of outcomes, we can calculate the expected scores and compare.
This leads us to a binomial probability distribution, where we can compute individual probabilities and sum accordingly to find the desired probability.