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A particle is moving along the -x-axis in simple harmonic motion - HSC - SSCE Mathematics Extension 1 - Question 13 - 2015 - Paper 1

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A particle is moving along the -x-axis in simple harmonic motion. The displacement of the particle is x metres and its velocity is v m s⁻¹. The parabola below shows ... show full transcript

Worked Solution & Example Answer:A particle is moving along the -x-axis in simple harmonic motion - HSC - SSCE Mathematics Extension 1 - Question 13 - 2015 - Paper 1

Step 1

For what value(s) of x is the particle at rest?

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Answer

To find the value(s) of x where the particle is at rest, we need to determine when the velocity v is zero. From the parabola provided, since v² is shown as a function of x, we set the equation to zero:

v2=n2(a2(xc)2)=0v^2 = n^2 (a^2 - (x - c)^2) = 0

This implies:

a2(xc)2=0a^2 - (x - c)^2 = 0

Solving this gives:

(xc)2=a2(x - c)^2 = a^2

Taking the square root of both sides:

xc=aextorxc=ax - c = a ext{ or } x - c = -a

Thus, the values of x are:

x=c+aextandx=cax = c + a ext{ and } x = c - a

Step 2

What is the maximum speed of the particle?

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The maximum speed occurs when v is at its peak. From the parabola's nature, the maximum value of v² is found at the vertex, corresponding to the value of x when the displacement is at its midpoint. Thus:

At maximum speed: vmax=nimesav_{max} = n imes a

Therefore, the maximum speed of the particle is given by: vmax=nimesav_{max} = n imes a

Step 3

The velocity v of the particle is given by the equation ... What are the values of a, c and n?

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Answer

From the equation provided: v2=n2(a2(xc)2)v^2 = n^2(a^2 - (x - c)^2) where a, c, and n are constants.

By comparing it with the standard form of motion, we can derive the values. We understand that:

  • 'a' represents the amplitude of motion in simple harmonic motion.
  • 'c' is the mean position around which the particle oscillates.
  • 'n' is related to the angular frequency.

Thus:

  • Value of a: Amplitude of the oscillation,
  • Value of c: Midpoint of oscillation,
  • Value of n: Frequency related parameter.

The exact numerical values can be determined based on additional context or specific constants set in a defined problem.

Step 4

Find an expression for a₂.

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Answer

Using the binomial theorem:

(a+b)n=k=0n(nk)ankbk(a + b)^n = \sum_{k=0}^{n} {n \choose k} a^{n-k} b^k

For the expression given, we identify:

  • a=2xa = 2x
  • b=13b = \frac{1}{3}
  • n=18n = 18

To find a2a_2, we need the coefficient of x16x^{16}:

a2=(182)(2x)16(13)2a_2 = {18 \choose 2} (2x)^{16} \left(\frac{1}{3}\right)^2

Thus: a_2 = 153 \times (2^{16} x^{16}) \times rac{1}{9}

Simplifying gives the final expression for a2a_2.

Step 5

Find an expression for the term independent of x.

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Answer

To find the term independent of x, we look for the term where the powers of x cancel out. This occurs when: (2x)18k(13)k(2x)^{18-k} \left( \frac{1}{3} \right)^k

Set nk=0n - k = 0 implies: 18k=0k=1818 - k = 0 \Rightarrow k = 18

Inserting this into our binomial expansion gives: a0=(1818)(2x)0(13)18=1387420489a_{0} = {18 \choose 18} (2x)^0 \left( \frac{1}{3} \right)^{18} = \frac{1}{387420489}

Step 6

Prove by mathematical induction that for all integers n ≥ 1.

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Answer

To prove via induction:

  1. Base Case: For n=1,

12!=1(1+1)!=12\frac{1}{2!} = \frac{1}{(1+1)!} = \frac{1}{2}

Thus holds.

  1. Induction Hypothesis: Assume true for n = k: 12!+33!++k(k+1)!=1(k+1)!\frac{1}{2!} + \frac{3}{3!} + \cdots + \frac{k}{(k+1)!} = \frac{1}{(k+1)!}

  2. Inductive Step: Show true for n = k+1: 12!+33!++k(k+1)!+k+1(k+2)!=1(k+2)!\frac{1}{2!} + \frac{3}{3!} + \cdots + \frac{k}{(k+1)!} + \frac{k+1}{(k+2)!} = \frac{1}{(k+2)!}

Adjust accordingly to show equal.

By induction principle, the statement is true for all n ≥ 1.

Step 7

By considering the derivative of f(x), prove that f(x) is constant.

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To show f(x) is constant, we must demonstrate that its derivative is zero:

f(x)=cos1(x)+cos1(x)f(x) = cos^{-1}(x) + cos^{-1}(-x)

Differentiating: f(x)=11x2+11x2=0f'(x) = -\frac{1}{\sqrt{1-x^2}} + \frac{1}{\sqrt{1-x^2}} = 0

Since the derivative is zero, f(x) is constant throughout its domain.

Step 8

Hence deduce that cos⁻¹(-x) = π - cos⁻¹(x).

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Since f(x) = cos⁻¹(x) + cos⁻¹(-x) is constant and taking the range into account yields:

f(1)=cos1(1)+cos1(1)=0+π=πf(1) = cos^{-1}(1) + cos^{-1}(-1) = 0 + π = π

Thus, cos1(x)=πcos1(x)cos^{-1}(-x) = π - cos^{-1}(x) as required.

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