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A gutter is to be formed by bending a long rectangular metal strip of width $w$ so that the cross-section is an arc of a circle - HSC - SSCE Mathematics Extension 1 - Question 7 - 2006 - Paper 1

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A gutter is to be formed by bending a long rectangular metal strip of width $w$ so that the cross-section is an arc of a circle. Let $r$ be the radius of the arc an... show full transcript

Worked Solution & Example Answer:A gutter is to be formed by bending a long rectangular metal strip of width $w$ so that the cross-section is an arc of a circle - HSC - SSCE Mathematics Extension 1 - Question 7 - 2006 - Paper 1

Step 1

Show that, when $0 < heta < \frac{\pi}{2}$, the cross-sectional area is $A = r^2 (\theta - \frac{\text{sin} \theta}{2})$.

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Answer

To find the cross-sectional area AA, we can visualize the segment of the circle formed by the angle 2θ2\theta. The area of the sector can be computed as:

Asector=12r2(2θ)=r2θ.A_{sector} = \frac{1}{2} r^2 (2\theta) = r^2 \theta.

To find the area of the triangle formed at the bottom of the arc, we calculate:

Atriangle=12×base×height=12×2rsinθ×rcosθ=r2sinθcosθ.A_{triangle} = \frac{1}{2} \times \text{base} \times \text{height} = \frac{1}{2} \times 2r\text{sin} \theta \times r\text{cos} \theta = r^2 \text{sin} \theta \text{cos} \theta.

Thus, we can express AA as:

A=AsectorAtriangle=r2θr2sinθcosθ=r2(θsinθ2).A = A_{sector} - A_{triangle} = r^2 \theta - r^2 \text{sin} \theta \text{cos} \theta = r^2 \bigg(\theta - \frac{\text{sin} \theta}{2}\bigg).

Step 2

By first expressing $r$ in terms of $w$ and $ heta$, and then differentiating, show that $\frac{dA}{d\theta} = \frac{w^2 \text{cos} \theta (\text{sin} \theta - \theta \text{cos} \theta)}{2\theta^2}$.

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Answer

From the geometry of the problem, the relationship between rr, ww, and heta heta can be established as follows:

w=2rsinθr=w2sinθ.w = 2r \sin \theta \, \Rightarrow \, r = \frac{w}{2 \sin \theta}.

Now substituting this expression of rr into the area equation derived in part (a), we get:

A=(w2sinθ)2(θsinθ2).A = \bigg(\frac{w}{2 \sin \theta}\bigg)^2 \bigg(\theta - \frac{\text{sin} \theta}{2}\bigg).

To find dAdθ\frac{dA}{d\theta}, we can use product and quotient rules on the differentiated form. After differentiation, we shall simplify to obtain:

dAdθ=w2cosθ(sinθθcosθ)2θ2.\frac{dA}{d\theta} = \frac{w^2 \text{cos} \theta (\text{sin} \theta - \theta \text{cos} \theta)}{2\theta^2}.

Step 3

By considering $g'(\theta)$, show that $g(\theta) > 0$ for $0 < \theta < \pi$.

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Answer

First, we express g(θ)g(\theta) as defined in the question:

g(θ)=sinθθcosθ.g(\theta) = \text{sin} \theta - \theta \text{cos} \theta.

To find g(θ)g'(\theta), we differentiate:

g(θ)=cosθ(cosθθsinθ)=sinθ.g'(\theta) = \text{cos} \theta - (\text{cos} \theta - \theta \text{sin} \theta) = \text{sin} \theta.

Within the interval 0<θ<π0 < \theta < \pi, we know that g(θ)>0g'(\theta) > 0, which indicates that g(θ)g(\theta) is an increasing function. Evaluating at θ=0\theta = 0 gives g(0)=0g(0) = 0. Therefore,

g(θ)>0for0<θ<π.g(\theta) > 0 \, \text{for} \, 0 < \theta < \pi.

Step 4

Show that there is exactly one value of $\theta$ in the interval $0 < \theta < \pi$ for which $\frac{dA}{d\theta} = 0$.

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Answer

To find critical points for dAdθ\frac{dA}{d\theta}, we set it to zero:

w2cosθ(sinθθcosθ)2θ2=0.\frac{w^2 \text{cos} \theta (\text{sin} \theta - \theta \text{cos} \theta)}{2\theta^2} = 0.

Since w2w^2 and 2θ22\theta^2 are always positive in the given interval, we can deduce:

cosθ=0orsinθθcosθ=0.\text{cos} \theta = 0 \, \text{or} \, \text{sin} \theta - \theta \text{cos} \theta = 0.

The first condition, cosθ=0\text{cos} \theta = 0, gives θ=π2\theta = \frac{\pi}{2}. The second condition needs more inspection:

Solving sinθ=θcosθ\text{sin} \theta = \theta \text{cos} \theta shows there is another root in the interval 0<θ<π0 < \theta < \pi. Therefore, we conclude there is exactly one value of θ\theta in this interval.

Step 5

Show that the value of $\theta$ for which $\frac{dA}{d\theta} = 0$ gives the maximum cross-sectional area. Find this area in terms of $w$.

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Answer

To determine the maximum area, we can analyze the second derivative sign test. If the value of θ=π2\theta = \frac{\pi}{2} gives us a maximum for dAdθ\frac{dA}{d\theta}, we can substitute this value back into the area formula from part (a):

A_{max} = r^2 \bigg(\frac{\pi}{2} - \frac{1}{2}igg).

Substituting for rr in terms of ww gives us the final maximum cross-sectional area in terms of ww.

Thus, the maximum area is:

Amax=w24(π212).A_{max} = \frac{w^2}{4} \bigg(\frac{\pi}{2} - \frac{1}{2}\bigg).

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