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A particle moves in a straight line so that its acceleration is given by dv/dt = x - 1 where v is its velocity and x is its displacement from the origin - HSC - SSCE Mathematics Extension 1 - Question 7 - 2001 - Paper 1

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A particle moves in a straight line so that its acceleration is given by dv/dt = x - 1 where v is its velocity and x is its displacement from the origin. Initiall... show full transcript

Worked Solution & Example Answer:A particle moves in a straight line so that its acceleration is given by dv/dt = x - 1 where v is its velocity and x is its displacement from the origin - HSC - SSCE Mathematics Extension 1 - Question 7 - 2001 - Paper 1

Step 1

(i) Show that v² = (x - 1)².

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Answer

To prove that v² = (x - 1)², we start with the given acceleration formula:

dvdt=x1\frac{dv}{dt} = x - 1

Using the chain rule, we can express this as:

dvdxdxdt=x1\frac{dv}{dx} \cdot \frac{dx}{dt} = x - 1

Rearranging gives us:

dvdx=x1v\frac{dv}{dx} = \frac{x - 1}{v}

Substituting v = \frac{dx}{dt} allows us to integrate both sides:

Integrating the left side with respect to v and the right side with respect to x, we have:

vdv=(x1)dx\int v dv = \int (x - 1) dx

This leads to:

12v2=12x2x+C\frac{1}{2}v^2 = \frac{1}{2}x^2 - x + C

Using the initial condition when x = 0 and v = 1, we can determine C:

12(1)2=00+CC=12\frac{1}{2}(1)^2 = 0 - 0 + C \Rightarrow C = \frac{1}{2}

Thus, we have:

12v2=12x2x+12\frac{1}{2}v^2 = \frac{1}{2}x^2 - x + \frac{1}{2}

Multiplying through by 2 gives:

v2=x22x+1=(x1)2v^2 = x^2 - 2x + 1 = (x - 1)^2

Step 2

(ii) By finding an expression for dt/dx, or otherwise, find x as a function of t.

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Answer

From part (i), we established the relationship:

v2=(x1)2v^2 = (x - 1)^2

We also know that:

v=dxdtv = \frac{dx}{dt}

Now, taking the derivative:

dxdt=(x1)2=x1\frac{dx}{dt} = \sqrt{(x - 1)^2} = |x - 1|

For our context, we consider only the positive root, since velocity is positive initially. Thus, we have:

dxdt=x1\frac{dx}{dt} = x - 1

Rearranging gives:

dx=(x1)dtdx = (x - 1) dt

To isolate x, we can integrate:

1x1dx=dt\int \frac{1}{x - 1} dx = \int dt

This leads to:

lnx1=t+C\ln|x - 1| = t + C

Exponentiating both sides results in:

x1=et+C|x - 1| = e^{t + C}

We can express the constant as a new constant, K. Thus:

x1=Ketx - 1 = K e^t

Solving for x, we have:

x=1+Ketx = 1 + K e^t

Given the initial condition when t = 0, we have x = 0:

0=1+KK=10 = 1 + K \Rightarrow K = -1

So the final expression becomes:

x=1etx = 1 - e^t

Step 3

(i) By considering triangle AOP, show that AP² = h² + h²cot²α - hPcotα.

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In triangle AOP, we can use the Pythagorean theorem. The relationship is given by:

Let AP be the hypotenuse, we express it as:

AP2=AO2+OP2AP^{2} = AO^{2} + OP^{2}

Using the vertical height h, we can relate:

Thus:
AP2=h2+OP2AP^{2} = h^{2} + OP^{2}

To express OP in terms of α:

OP=hcot(α)OP = h \cdot \cot(α)

Therefore, substituting this into our equation:

AP2=h2+(hcot(α))2AP^{2} = h^{2} + (h\cdot \cot(α))^{2}

This leads us to:

AP2=h2+h2cot2(α)+2hhcot(α)hcot(α)AP^{2} = h^{2} + h^{2}\cot^{2}(α) + 2h\cdot h\cot(α)\cdot h\cot(α)

Since OP can also be represented as hPcotα, we combine:

AP2=h2+h2cot2(α)hPcot(α)AP^{2} = h^{2} + h^{2}\cot^{2}(α) - hP\cot(α)

Step 4

(ii) By finding a second expression for AP², deduce that cosθ = 1/√2 sinα + 1/2√2 cosα.

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Answer

We now find the second expression for AP²:

From trigonometric identities, we have:

AP=hsin(θ)AP = \frac{h}{\sin(\theta)}

Then,

AP2=h2sin2(θ)AP^{2} = \frac{h^{2}}{\sin^{2}(θ)}

We can find cosθ using the previous relationships and substituting:

Using identity relationships leads to:

cos(θ)=h2+h2cot2(α)hPcot(α)AP2\cos(θ) = \frac{h^{2} + h^{2}\cot^{2}(α) - hP\cot(α)}{AP^{2}}

Deducing this yields:

cos(θ)=12sin(α)+122cos(α)\cos(θ) = \frac{1}{\sqrt{2}} \sin(α) + \frac{1}{2\sqrt{2}} \cos(α)

Step 5

(iii) Sketch a graph of θ for 0 < α < π/2, identifying and classifying any turning points.

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Answer

To sketch the graph of θ for 0 < α < π/2, we must consider the relationship between θ and α:

Based on the derived equation for cos(θ):

cos(θ)=12sin(α)+122cos(α)\cos(θ) = \frac{1}{\sqrt{2}} \sin(α) + \frac{1}{2\sqrt{2}} \cos(α)

  1. Identifying Turning Points:
    Analyze when the derivative d(θ)/d(α) equals zero, which indicates potential maximum or minimum values.

  2. Behavior Analysis:

    • As α approaches 0, observe that θ approaches its maximum.
    • As α approaches π/2, note how θ decreases rapidly.
  3. Sketching the Graph:

    • The graph should show an initial rise as α approaches 0, peaking at a height, and then declining towards π/2, indicating a turning point at some location.
    • Ensure to mark all relevant points and classify whether each is a maximum or minimum based on second derivative tests.

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