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A small bead of mass m is attached to one end of a light string of length R - HSC - SSCE Mathematics Extension 2 - Question 5 - 2011 - Paper 1

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A small bead of mass m is attached to one end of a light string of length R. The other end of the string is fixed at height 2h above the centre of a sphere of radius... show full transcript

Worked Solution & Example Answer:A small bead of mass m is attached to one end of a light string of length R - HSC - SSCE Mathematics Extension 2 - Question 5 - 2011 - Paper 1

Step 1

By resolving the forces horizontally and vertically on a diagram, show that

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Answer

To resolve the forces, we place the bead in equilibrium along both the horizontal and vertical axes. We have:

  1. Horizontal Resolution: The horizontal component of the tension in the string contributes to the circular motion, giving: FsinθNsinθ=mrF \, \sin{\theta} - N \, \sin{\theta} = m \, r

  2. Vertical Resolution: The vertical components of the forces give: Fcosθ+Ncosθ=mgF \, \cos{\theta} + N \, \cos{\theta} = mg

These equations represent equilibrium in the respective directions.

Step 2

Show that

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To show that N=12msecθ12mRrcscθ,N = \frac{1}{2} m \, \sec{\theta} - \frac{1}{2} m \frac{R}{r} \, \csc{\theta}, we start from the vertical resolution of forces.

  1. From the equation, we solve for N:

    • Isolate N in terms of F and other known quantities from the equations above.
    • By substituting the expression for F using the equations, we relate the terms accordingly.
  2. Simplifying further will lead to the required form.

Step 3

Show that the bead remains in contact with the sphere if ω ≤ √(g/h)

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To verify the condition:

  1. Use the derived formula for N and set up the inequality for it to remain non-negative: N0.N \geq 0.
  2. Substitute the expression for N obtained previously and solve the inequality for ω:
    • Recognizing that for contact maintenance, we need to ensure the gravitational influence balances with the angular momentum derived forces
    • Hence deducing the required relationship: if ( \omega \leq \sqrt{\frac{g}{h}} ), the bead remains in contact.

Step 4

Using a common denominator or multiplying both sides by (1 + p)(1 + q), then correctly simplifying the denominator to be \( p + q + r + 2pq + pr. \)

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We start with: p1+p+q1+q+r1+r.\frac{p}{1 + p} + \frac{q}{1 + q} + \frac{r}{1 + r}.

  1. Applying the common denominator, expand: p(1+q)(1+r)+q(1+p)(1+r)+r(1+p)(1+q)(1+p)(1+q)(1+r).\Rightarrow \frac{p(1 + q)(1 + r) + q(1 + p)(1 + r) + r(1 + p)(1 + q)}{(1 + p)(1 + q)(1 + r)}.
  2. Simplifying will yield:
    • Look carefully at how all interactions occur in terms of the positivity condition and arrive at the conclusion.

Step 5

Use the reflection property of the ellipse at P to prove that SQ = RQ.

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Using the reflection property of ellipses, which states that any ray from one focus reflects off the tangent line to the ellipse and passes through the other focus:

  1. At point P, any light ray coming from focus S reflects such that it passes through focus S'.
  2. Thus, we have:
    • The segments ( SQ ) and ( RQ ) are equal, confirming the property.

Step 6

Explain why S'R = 2a.

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From the ellipse definition, the distance between the foci is given by:

  • Using the properties of ellipses, the distance S'S relates to the semi-major axis a: SR=2a.S'R = 2a. This follows from properties of elliptical geometry that state distances involving foci and points on the ellipse return measures directly relative to semi-major axis.

Step 7

Hence, or otherwise, prove that Q lies on the circle x² + y² = a² at the point R.

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To show that point Q lies on the circle defined by the equation:

  1. Connect the properties established about distances from P, S, and S' to point Q.
  2. Demonstrate that under the relationships established, Q maintains a radial distance from the origin equivalent to a, thus proving: x2+y2=a2.x^{2} + y^{2} = a^{2}.

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