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Find the exact value of the volume of the solid of revolution formed when the region bounded by the curve $y = an(2x)$, the x-axis and the line $x = \frac{\pi}{8}$ is rotated about the x-axis - HSC - SSCE Mathematics Extension 1 - Question 5 - 2005 - Paper 1

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Find the exact value of the volume of the solid of revolution formed when the region bounded by the curve $y = an(2x)$, the x-axis and the line $x = \frac{\pi}{8}$ ... show full transcript

Worked Solution & Example Answer:Find the exact value of the volume of the solid of revolution formed when the region bounded by the curve $y = an(2x)$, the x-axis and the line $x = \frac{\pi}{8}$ is rotated about the x-axis - HSC - SSCE Mathematics Extension 1 - Question 5 - 2005 - Paper 1

Step 1

Find the exact value of the volume of the solid of revolution

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Answer

To find the volume of the solid of revolution generated by rotating the area under the curve y=an(2x)y = an(2x) from x=0x = 0 to x=π8x = \frac{\pi}{8} about the x-axis, we can use the formula: V=πab[f(x)]2dxV = \pi \int_a^b [f(x)]^2 \, dx

In this case:

  • f(x)=tan(2x)f(x) = \tan(2x)
  • The limits of integration are a=0a = 0 and b=π8b = \frac{\pi}{8}.

Thus the volume can be calculated as: V=π0π8[tan(2x)]2dxV = \pi \int_0^{\frac{\pi}{8}} [\tan(2x)]^2 \, dx Using the identity tan2u=sec2u1\tan^2 u = \sec^2 u - 1, we substitute: V=π0π8(sec2(2x)1)dxV = \pi \int_0^{\frac{\pi}{8}} (\sec^2(2x) - 1) \, dx Calculating this integral will yield the exact volume.

Step 2

Explain why DP AE is a cyclic quadrilateral

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Answer

A cyclic quadrilateral is defined as a quadrilateral whose vertices all lie on the circumference of a circle. In this case, quadrilateral DP AE is cyclic because the points D, P, A, and E all lie on the circumference of the circle defined by points A and B, thus satisfying the condition of a cyclic quadrilateral.

Step 3

Prove that $\angle APE = \angle ABC$

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Answer

To prove that the angles are equal, we can use the property of angles subtended by the same arc in a circle. Since points A, P, E, and B lie on the arc AB, it follows that: APE=ABC\angle APE = \angle ABC This holds because both angles subtend the same chord AB of the circle.

Step 4

Deduce that PQ is perpendicular to BC

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Answer

Since we have established that APE=ABC\angle APE = \angle ABC and both angles are subtended from points A and E, we can deduce that lines AP and BC are perpendicular to one another at point P. Thus, it follows that the line PQ is perpendicular to BC, given that it extends vertically from point P down to line BC.

Step 5

Express $\sqrt{3}\sin(3t) - \cos(3t)$ in the form R sin(3t - α)

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Answer

We express the linear combination of sine and cosine in the form Rsin(3tα)R \sin(3t - \alpha). To find R and α, we compare:

  1. Find R using the formula: R=A2+B2R = \sqrt{A^2 + B^2} where A=3A = \sqrt{3} and B=1B = -1. Thus: R=(3)2+(1)2=3+1=2R = \sqrt{(\sqrt{3})^2 + (-1)^2} = \sqrt{3 + 1} = 2
  2. To find α, we use the relationship: tan(α)=13\tan(\alpha) = \frac{-1}{\sqrt{3}} This gives α=π3\alpha = \frac{\pi}{3}, thus: 3sin(3t)cos(3t)=2sin(3tπ3)\sqrt{3}\sin(3t) - \cos(3t) = 2\sin(3t - \frac{\pi}{3})

Step 6

Find the amplitude and the period of the oscillation.

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Answer

The amplitude of the simple harmonic motion is given by R, which we found to be 2. The period T can be calculated from the angular frequency ω: Since the function x=5+2sin(3tπ3)x = 5 + 2 \sin(3t - \frac{\pi}{3}), the angular frequency is 3: T=2πω=2π3T = \frac{2\pi}{\omega} = \frac{2\pi}{3}

Step 7

Calculate the maximum speed when v = 0

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Answer

The speed of the particle can be derived from the position function by taking the derivative: v=dxdtv = \frac{dx}{dt} Calculating the derivative and setting it to zero allows us to find the maximum speed:

  1. Differentiate x=5+2sin(3tπ3)x = 5 + 2\sin(3t - \frac{\pi}{3}): v(t)=6cos(3tπ3)v(t) = 6\cos(3t - \frac{\pi}{3})
  2. To find when v=0v = 0 we solve: 6cos(3tπ3)=06\cos(3t - \frac{\pi}{3}) = 0 This occurs when: 3tπ3=π2+nπ,nZ3t - \frac{\pi}{3} = \frac{\pi}{2} + n\pi, n \in \mathbb{Z} From this we can determine the times at which the speed reaches its maximum.

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