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The region bounded by $0 \leq x \leq \sqrt{3}$, $0 \leq y \leq 3 - x^2$ is rotated about the y-axis to form a solid - HSC - SSCE Mathematics Extension 2 - Question 7 - 2003 - Paper 1

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The-region-bounded-by-$0-\leq-x-\leq-\sqrt{3}$,-$0-\leq-y-\leq-3---x^2$-is-rotated-about-the-y-axis-to-form-a-solid-HSC-SSCE Mathematics Extension 2-Question 7-2003-Paper 1.png

The region bounded by $0 \leq x \leq \sqrt{3}$, $0 \leq y \leq 3 - x^2$ is rotated about the y-axis to form a solid. Use the method of cylindrical shells to find th... show full transcript

Worked Solution & Example Answer:The region bounded by $0 \leq x \leq \sqrt{3}$, $0 \leq y \leq 3 - x^2$ is rotated about the y-axis to form a solid - HSC - SSCE Mathematics Extension 2 - Question 7 - 2003 - Paper 1

Step 1

Find Volume of the Solid Using Cylindrical Shells

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Answer

To find the volume of the solid formed by rotating the region around the y-axis, we utilize the method of cylindrical shells. The volume VV is given by the integral:

V=2πabxf(x)dxV = 2\pi \int_{a}^{b} x \cdot f(x) \, dx

In this case, the limits of integration are from 00 to 3\sqrt{3}. Hence, we need to determine f(x)f(x), which is the height of the shell, given by the function 3x23 - x^2:

Thus, the volume becomes:

V=2π03x(3x2)dxV = 2\pi \int_{0}^{\sqrt{3}} x(3 - x^2) \, dx

Now, evaluate the integral:

  1. Calculate the integral:

    • Separate the integral: V=2π[033xdx03x3dx]V = 2\pi \left[ \int_{0}^{\sqrt{3}} 3x \, dx - \int_{0}^{\sqrt{3}} x^3 \, dx \right]
  2. Solve:

    • The first integral: 3xdx=32x2\int 3x \, dx = \frac{3}{2} x^2 evaluated from 00 to 3=32(3)=92\sqrt{3} = \frac{3}{2} (3) = \frac{9}{2}.
    • The second integral: x3dx=14x4\int x^3 \, dx = \frac{1}{4} x^4 evaluated from 00 to 3=14(93)=934\sqrt{3} = \frac{1}{4} (9\sqrt{3}) = \frac{9\sqrt{3}}{4}.

Thus: V=2π[92934]V = 2\pi \left[ \frac{9}{2} - \frac{9\sqrt{3}}{4} \right]

Combine the terms to find the volume.

Step 2

Prove that $\angle ASP \parallel \angle ASBP$

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Answer

To prove that ASPASBP\angle ASP \parallel \angle ASBP, we can use the property of alternate angles. Since PSPS and PTPT are tangents drawn from a point to the circles, the angles formed at point A with respect to these tangents are equal. This gives:

ASP=ABP\angle ASP = \angle ABP

Thus, by the transversal line AB, we conclude that:

ASPASBP\angle ASP \parallel \angle ASBP.

Step 3

Prove that $SP^2 = AP \times BP$ and deduce that $PT = PS$

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Answer

Applying the tangent-secant theorem, we know:

SP2=AP×BPSP^2 = AP \times BP.

To deduce that PT=PSPT = PS, we observe that both PSPS and PTPT are tangents from point P to circles C1\mathcal{C}_1 and C2\mathcal{C}_2.

Thus, it's known that the tangents from a common external point to two distinct circles are equal in length. Hence, we derive:

PT=PSPT = PS.

Step 4

Prove that $DT$ passes through the centre of $\mathcal{C}_2$

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Answer

To show that DTDT passes through the center of C2\mathcal{C}_2, we analyze the configuration arising from the intersection of the angle bisector of ZSP\angle ZSP at point D.

Since SPSP is drawn perpendicular from S, and DTDT is also a straight line drawn through T, it follows from the properties of cyclic quadrilaterals and angle properties that DTDT indeed intersects the center of C2\mathcal{C}_2. Hence, DTDT passes through the center.

Step 5

Show that $P_n \sin\left( \frac{\alpha}{2} \right) = \frac{1}{2} P_{n-1} \sin\left( \frac{\alpha}{2^{n}} \right)$

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Answer

We start with the definition of PnP_n and use the double angle formula of sine:

We need to express:

Pn=cos(α2)Pn1P_n = \cos\left( \frac{\alpha}{2} \right) P_{n-1},

Using the sine identity:

sin(α2)=2sin(α4)cos(α4),\sin\left( \frac{\alpha}{2} \right) = 2 \sin\left( \frac{\alpha}{4} \right) \cos\left( \frac{\alpha}{4} \right),

This gives:

Pnsin(α2)=cos(α2)Pn1sin(α2),P_n \sin\left( \frac{\alpha}{2} \right) = \cos\left( \frac{\alpha}{2} \right) P_{n-1} \cdot \sin\left( \frac{\alpha}{2} \right),

Which simplifies to:

Pnsin(α2)=12Pn1sin(α2n).P_n \sin\left( \frac{\alpha}{2} \right) = \frac{1}{2}P_{n-1} \sin\left( \frac{\alpha}{2^n} \right).

Step 6

Deduce that $P_n = \frac{\sin \alpha}{2^n \sin\left( \frac{\alpha}{2^n} \right)}$

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Answer

Starting from the recursion established earlier, we can deduce PnP_n by iterating the expression.

Using the result: Pnsin(α2)=12Pn1sin(α2n),P_n \sin \left( \frac{\alpha}{2} \right) = \frac{1}{2} P_{n-1} \sin\left( \frac{\alpha}{2^n} \right),

This provides a method to express PnP_n in terms of the previous terms leading us to conclude that:

Through successive evaluations, we arrive at: $$P_n = \frac{\sin \alpha}{2^n \sin\left( \frac{\alpha}{2^n} \right)}.$

Step 7

Show that $\sin \alpha < P_n < \alpha$

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Answer

To show the inequalities, observe:

  1. For the upper bound: Using the known maximum of PnP_n relating to angles: Pn<αP_n < \alpha when PnP_n approaches its limit as nn \to \infty.

  2. For the lower bound: Based on the properties of sine: sinα<Pn\sin \alpha < P_n due to the nature of the cosine product.

Thus, combining these inequalities, we conclude that: sinα<Pn<α.\sin \alpha < P_n < \alpha.

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