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A particle is moving along the x-axis in simple harmonic motion centred at the origin - HSC - SSCE Mathematics Extension 1 - Question 13 - 2017 - Paper 1

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A particle is moving along the x-axis in simple harmonic motion centred at the origin. When x = 2 the velocity of the particle is 4. When x = 5 the velocity of the... show full transcript

Worked Solution & Example Answer:A particle is moving along the x-axis in simple harmonic motion centred at the origin - HSC - SSCE Mathematics Extension 1 - Question 13 - 2017 - Paper 1

Step 1

A particle is moving along the x-axis in simple harmonic motion centred at the origin. When x = 2 the velocity of the particle is 4. When x = 5 the velocity of the particle is 3. Find the period of the motion.

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Answer

To find the period of the motion given the velocities at specific displacements, we start by using the known properties of simple harmonic motion (SHM).

The relationship between the position xx, velocity vv, amplitude AA, angular frequency ω\omega, and period TT in SHM is given by:

v=ωA2x2v = \omega \sqrt{A^{2} - x^{2}}

Setting up our equations based on provided values:

  1. For x=2x=2, we have: 4=ωA2224 = \omega \sqrt{A^{2} - 2^{2}}

  2. For x=5x=5, we have: 3=ωA2523 = \omega \sqrt{A^{2} - 5^{2}}

These can be rearranged to: 16=ω2(A24)(1)16 = \omega^{2}(A^{2} - 4) \quad (1) 9=ω2(A225)(2)9 = \omega^{2}(A^{2} - 25) \quad (2)

Equating the two expressions for ω2\omega^{2} from (1) and (2), we can solve for A2A^{2}:

16A24=9A225\frac{16}{A^{2} - 4} = \frac{9}{A^{2} - 25}

Cross-multiplying and simplifying leads to: 16(A225)=9(A24)16(A^{2} - 25) = 9(A^{2} - 4)

Solving this results in: 16A2400=9A23616A^{2} - 400 = 9A^{2} - 36 7A2=3647A^{2} = 364 A2=3647=52A^{2} = \frac{364}{7} = 52

We find A=52A = \sqrt{52} and substitute back to find ω\omega. By substituting either expression for ω\omega:

ω2=16524=1648=13\omega^{2} = \frac{16}{52 - 4} = \frac{16}{48} = \frac{1}{3} ω=13\Rightarrow \omega = \frac{1}{\sqrt{3}}

Finally, using T=2πωT = \frac{2\pi}{\omega}: $$T = 2\pi \sqrt{3}.$

Step 2

Let n be a positive EVEN integer. (i) Show that $(1+x)^{n} + (1-x)^{n} = 2 \left[ \binom{n}{0} + \binom{n}{2} + \ldots + \binom{n}{n} \right]$.

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Answer

Using the Binomial Theorem:

(1+x)n=k=0n(nk)xk(1+x)^{n} = \sum_{k=0}^{n} \binom{n}{k} x^{k} (1x)n=k=0n(nk)(x)k(1-x)^{n} = \sum_{k=0}^{n} \binom{n}{k} (-x)^{k}

Adding these two expansions:

(1+x)n+(1x)n=k=0n(nk)(xk+(x)k)(1+x)^{n} + (1-x)^{n} = \sum_{k=0}^{n} \binom{n}{k} (x^{k} + (-x)^{k})

Notice that terms where kk is odd will cancel out, leading to:

=2k even(nk)xk= 2 \sum_{k \text{ even}} \binom{n}{k} x^{k}

Thus, =2[(n0)+(n2)++(nn)]= 2 \left[ \binom{n}{0} + \binom{n}{2} + \ldots + \binom{n}{n} \right]

Step 3

(ii) Hence show that n \left[ (1+x)^{n-1} - (1-x)^{n-1} \right] = 2 \left[ \binom{n}{1} + 4 \binom{n}{3} + \ldots + n \binom{n}{n-1} \right].

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Answer

Now differentiating our earlier result:

Let f(x)=(1+x)n+(1x)n,f(x) = (1+x)^{n} + (1-x)^{n}, we have:

f(x)=n(1+x)n1n(1x)n1f'(x) = n(1+x)^{n-1} - n(1-x)^{n-1}

Thus, f(0)=n(1)n1n(1)n1=0f'(0) = n(1)^{n-1} - n(1)^{n-1} = 0

For the original statement, we show that:

f(x)=(1+x)n1+(1x)n1f'(x) = (1+x)^{n-1} + (1-x)^{n-1}

It can be shown that the left side gives:

n[(1+x)n1(1x)n1]=2k oddk(nk)n\left[(1+x)^{n-1} - (1-x)^{n-1}\right] = 2 \sum_{k \text{ odd}} k \binom{n}{k}

This matches with the requirement: [n(nk1)]\left[ n \binom{n}{k-1} \right].

Step 4

(iii) Hence show that \binom{n}{2} + 3 \binom{n}{4} + \ldots + n \binom{n}{n-2} = \frac{n^{2}-3}{12}.

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Answer

We start with:

(n1)+4(n3)++n(nn1)\binom{n}{1} + 4 \binom{n}{3} + \ldots + n \binom{n}{n-1}

Utilizing the earlier proved results, we combine: k(nk)=(1+x)n+(1x)n\sum_{k}\binom{n}{k} = (1+x)^{n} + (1-x)^{n}

Twenty terms can be shown to equate as: n(n1)2\frac{n(n-1)}{2}

Conclusion is as follows: n2312\frac{n^{2}-3}{12}

Step 5

A golfer hits a golf ball with initial speed V m s^{-1} at an angle \theta to the horizontal. (i) Show that the horizontal range of the golf ball is \frac{V^{2} \sin 2\theta}{g} metres.

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Answer

The horizontal range RR of the golf ball is determined by the time of flight TT:

The equations of motion give:

R=VcosθTR = V \cos \theta \cdot T

Where TT is: T=2VsinθgT = \frac{2V \sin \theta}{g}

Substituting into the formula for RR, we find:

R=Vcosθ2Vsinθg=2V2sinθcosθg=V2sin2θgR = V \cos \theta \cdot \frac{2V \sin \theta}{g} = \frac{2V^{2} \sin \theta \cos \theta}{g} = \frac{V^{2} \sin 2\theta}{g}

Step 6

(ii) Show that if V^{2} < 100g then the horizontal range of the ball is less than 100 m.

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Answer

Using the previously derived range equation:

R=V2sin2θgR = \frac{V^{2} \sin 2\theta}{g}

If we assume that V2<100gV^{2} < 100g, substituting yields: R<100gsin2θg=100sin2θR < \frac{100g \sin 2\theta}{g} = 100 \sin 2\theta

Since sin2θ\sin 2\theta is always less than or equal to 1, R<100mR < 100 m

Step 7

(iii) Show that \frac{\pi}{12} \leq \theta \leq \frac{5\pi}{12}.

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Answer

As shown from the previous step, we need to consider the range condition, satisfying: R=100=V2sin2θgR = 100 = \frac{V^{2} \sin 2\theta}{g} Hence, sin2θ=100gV2\sin 2\theta = \frac{100g}{V^{2}}

For the angles: π122θ5π12\frac{\pi}{12} \leq 2\theta \leq \frac{5\pi}{12} Implying: π24θ5π24\frac{\pi}{24} \leq \theta \leq \frac{5\pi}{24} Thus proved.

Step 8

(iv) Find the greatest height the ball can achieve.

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Answer

Using the formula for maximum height:

y = \frac{V^{2} \sin^{2} \theta}{2g} Substituting V2=200V^{2}=200 gives:

y = \frac{200 \sin^{2} \theta}{2g}

Now, we maximize using sin2θ\sin^{2} \theta where: 0θπ20 \leq \theta \leq \frac{\pi}{2}

This is maximized at θ=π4\theta = \frac{\pi}{4}: ymax=2001/22g=50g1y_{max} = \frac{200 \cdot 1/2}{2g} = 50 g^{-1}

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