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

Worked Solution & Example Answer:12. 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 a particle in simple harmonic motion, we need to determine the period of the motion. The displacement function is given by

x=2extsin3tx = 2 ext{sin } 3t.

To find the period TT, we use the coefficient of tt inside the sine function:

T = rac{2 ext{π}}{ ext{frequency}} = rac{2 ext{π}}{3}.

Thus, the time at which the particle first returns to the origin (where x=0x = 0) is at the end of the first half of the period, or rac{T}{2} = rac{ ext{π}}{3}.

The total distance travelled to return to the origin is twice the amplitude of the motion, hence:

$$ ext{Distance} = 2 imes 2 = 4 ext{ metres}.$

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 zero. The velocity is derived from the displacement function:

v = rac{dx}{dt} = 2 imes 3 ext{cos}(3t) = 6 ext{cos}(3t).

Setting v=0v = 0 gives:

6extcos(3t)=0extcos(3t)=0.6 ext{cos}(3t) = 0 \Rightarrow ext{cos}(3t) = 0.

This occurs at:

3t = rac{ ext{π}}{2}, \Rightarrow t = rac{ ext{π}}{6}.

To find the acceleration, we differentiate the velocity:

a = rac{dv}{dt} = -6 imes 3 ext{sin}(3t) = -18 ext{sin}(3t).

Substituting t = rac{ ext{π}}{6} gives:

$$a = -18 ext{sin}igg(3 imes rac{ ext{π}}{6}igg) = -18 ext{sin}igg( rac{ ext{π}}{2}igg) = -18 imes 1 = -18 ext{ 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=extcos4xy = ext{cos } 4x about the xx-axis, we use the formula for the volume of revolution:

V=extπab[f(x)]2dx,V = ext{π} \int_{a}^{b} [f(x)]^2 \, dx,

where f(x)=extcos4xf(x) = ext{cos } 4x, a=0a = 0, and b = rac{ ext{π}}{2}. Thus,

V = ext{π} \int_{0}^{ rac{ ext{π}}{2}} ( ext{cos } 4x)^2 \, dx.

Using the double angle formula, we have:

( ext{cos } 4x)^2 = rac{1 + ext{cos } 8x}{2}.

Therefore,

V = ext{π} \int_{0}^{ rac{ ext{π}}{2}} rac{1 + ext{cos } 8x}{2} \, dx = rac{ ext{π}}{2} \int_{0}^{ rac{ ext{π}}{2}} (1 + ext{cos } 8x) \, dx.

Calculating the integral gives:

$$V = rac{ ext{π}}{2} \left[x + rac{1}{8} ext{sin } 8x \right]_{0}^{ rac{ ext{π}}{2}} = rac{ ext{π}}{2} \left[ rac{ ext{π}}{2} + 0 - (0 + 0)\right] = rac{ ext{π}^2}{4}.$

Step 4

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

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Answer

To express v2v^2 in terms of xx, we start from the equation for acceleration:

rac{d^2x}{dt^2} = 2 - rac{x}{2}.

We have: rac{dv}{dt} = rac{dx}{dt} \times rac{dv}{dx} \Rightarrow v \frac{dv}{dx} = 2 - rac{x}{2}.

This gives us a first order separable equation:

v \frac{dv}{dx} = 2 - rac{x}{2}.

Integrating both sides:

vdv=(2x2)dx\int v \, dv = \int (2 - \frac{x}{2}) \, dx

which results in

12v2=2x14x2+C.\frac{1}{2}v^2 = 2x - \frac{1}{4}x^2 + C.

Using the condition v=4v = 4 when x=0x = 0:

12(4)2=0+CC=8.\frac{1}{2}(4)^2 = 0 + C \Rightarrow C = 8.

Thus,

12v2=2x14x2+8.\frac{1}{2}v^2 = 2x - \frac{1}{4}x^2 + 8.

Finally, multiplying by 2 yields:

v2=4x12x2+16.v^2 = 4x - \frac{1}{2}x^2 + 16.

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