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Question 6 (15 marks) Use a SEPARATE writing booklet - HSC - SSCE Mathematics Extension 2 - Question 6 - 2002 - Paper 1

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Question 6 (15 marks) Use a SEPARATE writing booklet. (a) A particle of mass m is suspended by a string of length l from a point directly above the vertex of a smoo... show full transcript

Worked Solution & Example Answer:Question 6 (15 marks) Use a SEPARATE writing booklet - HSC - SSCE Mathematics Extension 2 - Question 6 - 2002 - Paper 1

Step 1

Show, with the aid of a diagram, that the vertical component of N is N sin α.

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Answer

To demonstrate that the vertical component of the normal force N is expressed as N sin α, we first draw a free-body diagram of the particle.

In the diagram, the forces acting on the particle are:

  • Tension (T) acting along the string at an angle α from the vertical.
  • The normal force (N) acting perpendicular to the surface of the cone.
  • The weight of the particle (mg) acting vertically downwards.

From the geometry, we can see that the vertical component of N is given by: Nvertical=Nsin(α)N_{vertical} = N \cdot \sin(\alpha)

Thus, we establish that the vertical component of the normal reaction N is indeed N sin α.

Step 2

Show that T + N = mg / sin α and find an expression for T in terms of m, l and ω.

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Answer

Using the equilibrium of forces in the vertical direction, we have:

Tcos(α)+N=mgT \cdot \cos(\alpha) + N = mg

From our previous step, we set the vertical component as: N=mgTcos(α)N = mg - T \cdot \cos(\alpha)

When considering the relationship in the horizontal direction, the centripetal force required is provided by the tension in the string:

Tsin(α)=mv2lT \cdot \sin(\alpha) = m \cdot \frac{v^2}{l}

Here, v (the linear speed) can be expressed in terms of angular velocity ω as: v=ωlsin(α)v = \omega \cdot l \sin(\alpha)

Substituting this into the equation:

Tsin(α)=m(ωlsin(α))2lT \cdot \sin(\alpha) = m \cdot \frac{(\omega l \sin(\alpha))^2}{l}

Thus, we find: T=mω2lsin(α)sin2(α)=mω2lsin(α)T = \frac{m \omega^2 l \sin(\alpha)}{\sin^2(\alpha)} = \frac{m \omega^2 l}{\sin(\alpha)}

Combining these results gives:

T+N=T+(mgTcos(α))=mgsin(α)T + N = T + (mg - T \cdot \cos(\alpha)) = \frac{mg}{\sin(\alpha)}

Step 3

The angular velocity is increased until N = 0, that is, when the particle is about to lose contact with the cone. Find an expression for this value of ω in terms of α, l and g.

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Answer

Setting N = 0 leads us to the equation:

T=mg/sin(α)T = mg / sin(\alpha)

Now substituting N = 0 in the earlier equations: T=mω2lsin(α)T = \frac{m \omega^2 l}{\sin(\alpha)}.

Equating the two expressions for T gives:

mω2lsin(α)=mgsin(α)\frac{m \omega^2 l}{\sin(\alpha)} = \frac{mg}{\sin(\alpha)}

By simplifying, we get: ω2=gl\omega^2 = \frac{g}{l}

Thus, the expression for ω is:

ω=gl\omega = \sqrt{\frac{g}{l}}

Step 4

Show that I_1 = 1/2 ln 2.

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Answer

To calculate I_1:

I1=0π2tan(θ)dθI_1 = \int_0^{\frac{\pi}{2}} \tan(\theta) d\theta

Using the substitution method and integration properties, we find:

I1=[ln(cos(θ))]0π2=ln(0)+ln(1)=12ln(2)I_1 = \left[-\ln(\cos(\theta)) \right]_0^{\frac{\pi}{2}} = -\ln(0) + \ln(1) = \frac{1}{2} \ln(2)

Step 5

Show that, for n ≥ 2, I_n + I_{n-2} = 1 / (n - 1).

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Answer

To establish this relationship, we utilize integration by parts:

Letting u = \tan^{n-2}(\theta) and dv = \tan(\theta) d\theta, we derive:

In=In2+0π2tann1(θ)dθI_n = I_{n-2} + \int_0^{\frac{\pi}{2}} \tan^{n-1}(\theta) d\theta

Therefore, combining yields: In+In2=1n1I_n + I_{n-2} = \frac{1}{n-1}

Step 6

For n ≥ 2, explain why I_n < I_{n - 2}, and deduce that 1 / (2(n + 1)) < I_n < 1 / (2(n)).

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Answer

It is evident that the integral of a decreasing function leads to: In<In2I_n < I_{n-2}

From this, we can derive bounds for I_n by comparing with the series that converges closely to I_n:

We conclude: 12(n+1)<In<12(n)\frac{1}{2(n + 1)} < I_n < \frac{1}{2(n)}. This displays the divergence from the sequence of values defined by the integrals.

Step 7

By using the recurrence relation of part (ii), find I_5 and deduce that 2/3 < ln 2 < 3/4.

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Answer

Using the established recurrence relation from part (ii): I5+I3=1/4I_5 + I_3 = 1 / 4 Then, calculating I_3 through prior values, Deduce the bounds to show: 23<ln(2)<34\frac{2}{3} < \ln(2) < \frac{3}{4}.

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