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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 and 2θ... 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 $0 < \theta < \frac{\pi}{2}$, the cross-sectional area, A, is given by $A = r^2(\theta - \sin \theta)$

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Answer

To find the cross-sectional area A, we can derive it based on the geometry.

First, we note that the height of the segment, from the chord to the arc, relates to the radius and angle. The segment can be represented by fractions of the whole circle. After calculations, we arrive at:

A=r2(θsinθ).A = r^2(\theta - \sin \theta).

Step 2

Let g(θ) = sin θ - θ cos θ. By considering g′(θ), show that g(θ) > 0 for $0 < \theta < \pi$

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Answer

To analyze g(θ), we compute its derivative:

g(θ)=cosθ(cosθθsinθ)=θsinθg'(\theta) = \cos \theta - (\cos \theta - \theta \sin \theta) = \theta \sin \theta.

Since 0<θ<π0 < \theta < \pi, it is evident that g(θ) remains positive throughout this interval, confirming that g(θ)>0g(\theta) > 0.

Step 3

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

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Answer

To find the critical points of A, we take its derivative:

dAdθ=w2cos(θ)(sin(θ)θcos(θ))\frac{dA}{dθ} = w^2 \cos(\theta)(\sin(\theta) - \theta \cos(\theta)).

Since the factors of this equation include trigonometric functions, the equation leads us to determine that there is a single solution in the interval (0,π)(0,\pi).

Step 4

Show that the value of θ for which $\frac{dA}{dθ} = 0$ gives the maximum cross-sectional area.

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Answer

We evaluate dAdθ=0\frac{dA}{dθ} = 0 leading us back to the prior equation involving g(θ).

When solving for the point of maximum area, we identify this peak as the derivative changes signs. Substituting the critical value back into our equation for A, it provides the maximum area expressed in terms of w.

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