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
Question 5
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:
Horizontal Resolution: The horizontal component of the tension in the string contributes to the circular motion, giving:
Fsinθ−Nsinθ=mr
Vertical Resolution: The vertical components of the forces give:
Fcosθ+Ncosθ=mg
These equations represent equilibrium in the respective directions.
Step 2
Show that
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Answer
To show that
N=21msecθ−21mrRcscθ,
we start from the vertical resolution of forces.
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.
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:
Use the derived formula for N and set up the inequality for it to remain non-negative:
N≥0.
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:
1+pp+1+qq+1+rr.
Applying the common denominator, expand:
⇒(1+p)(1+q)(1+r)p(1+q)(1+r)+q(1+p)(1+r)+r(1+p)(1+q).
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:
At point P, any light ray coming from focus S reflects such that it passes through focus S'.
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:
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:
Connect the properties established about distances from P, S, and S' to point Q.
Demonstrate that under the relationships established, Q maintains a radial distance from the origin equivalent to a, thus proving:
x2+y2=a2.