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A particle is moving in simple harmonic motion about the origin, with displacement $x$ metres - HSC - SSCE Mathematics Extension 1 - Question 12 - 2014 - Paper 1

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A particle is moving in simple harmonic motion about the origin, with displacement $x$ metres. The displacement is given by $x = 2 \sin 3t$, where $t$ is time in sec... show full transcript

Worked Solution & Example Answer:A particle is moving in simple harmonic motion about the origin, with displacement $x$ metres - HSC - SSCE Mathematics Extension 1 - Question 12 - 2014 - Paper 1

Step 1

What is the total distance travelled by the particle when it first returns to the origin?

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Answer

To find the total distance travelled by the particle when it first returns to the origin, we need to determine the period of the motion. The given displacement is:

x(t)=2sin(3t)x(t) = 2 \sin(3t)

The amplitude is 2 m, and the motion is simple harmonic. The period TT can be calculated as:

T=2πω=2π3T = \frac{2\pi}{\omega} = \frac{2\pi}{3}

The particle returns to the origin after a full cycle, which implies that the total distance is:

Total Distance=4 m\text{Total Distance} = 4 \text{ m}

(since the particle goes from 0 to 2 m and back to 0, making the total path = 4 m).

Step 2

What is the acceleration of the particle when it is first at rest?

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Answer

The particle is at rest when its velocity is 0. The velocity can be found by differentiating the displacement function:

v(t)=dxdt=23cos(3t)=6cos(3t)v(t) = \frac{dx}{dt} = 2 \cdot 3 \cos(3t) = 6 \cos(3t)

Setting this equal to 0 gives:

6cos(3t)=0cos(3t)=06 \cos(3t) = 0 \Rightarrow \cos(3t) = 0

The first instance occurs when:

3t=π2t=π63t = \frac{\pi}{2} \Rightarrow t = \frac{\pi}{6}

Then we calculate the acceleration, which is the second derivative of displacement:

x¨(t)=d2xdt2=232sin(3t)=18sin(3t)\ddot{x}(t) = \frac{d^2x}{dt^2} = -2 \cdot 3^2 \sin(3t) = -18 \sin(3t)

Substituting t=π6t = \frac{\pi}{6} gives:

x¨=18sin(π2)=18\ddot{x} = -18 \sin\left(\frac{\pi}{2}\right) = -18

Therefore, the acceleration when the particle is first at rest is:

18 m/s2-18 \text{ m/s}^2.

Step 3

Find the volume of the solid.

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Answer

To find the volume of the solid formed by rotating the region bounded by y=cos4xy = \cos 4x and the xx-axis about the xx-axis, we use the disk method:

V=π0π(cos4x)2dxV = \pi \int_{0}^{\pi} (\cos 4x)^2 \, dx

Using the identity cos2θ=1+cos(2θ)2\cos^2 \theta = \frac{1 + \cos(2\theta)}{2}, we have:

V=π0π1+cos(8x)2dxV = \pi \int_{0}^{\pi} \frac{1 + \cos(8x)}{2} \, dx

Calculating the integral:

V=π2[x+sin(8x)8]0π=π2[π+0(0)]=π22V = \frac{\pi}{2} \left[ x + \frac{\sin(8x)}{8} \right]_{0}^{\pi} = \frac{\pi}{2} \left[ \pi + 0 - (0) \right] = \frac{\pi^2}{2}

Thus, the volume of the solid formed by the rotation is:

$$\frac{\pi^2}{2} \text{ cubic units}.$

Step 4

Given that v = 4 when x = 0, express v^2 in terms of x.

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Answer

Starting with the acceleration given by:

x¨=2x2\ddot{x} = 2 - \frac{x}{2}

Acceleration can also be expressed using velocity:

x¨=dvdt=dvdxdxdt=vdvdx\ddot{x} = \frac{dv}{dt} = \frac{dv}{dx} \cdot \frac{dx}{dt} = v \frac{dv}{dx}

Setting the two expressions for acceleration equal, we have:

vdvdx=2x2v \frac{dv}{dx} = 2 - \frac{x}{2}

Separating variables yields:

vdv=(2x2)dxvdv = \left(2 - \frac{x}{2}\right)dx

Integrating both sides leads to:

12v2=2xx24+C\frac{1}{2} v^2 = 2x - \frac{x^2}{4} + C

Using the boundary condition v=4v = 4 when x=0x = 0, we find:

ightarrow C = 8$$ Thus, we can express: $$\frac{1}{2} v^2 = 2x - \frac{x^2}{4} + 8$$ Therefore: $$v^2 = 4x - \frac{x^2}{2} + 16$$

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