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Let $\alpha$, $\beta$ and $\gamma$ be the three roots of $x^3 + px + q = 0$, and define $s_n$ by $$s_n = \alpha^n + \beta^n + \gamma^n \quad \text{for } n = 1, 2, 3, \ldots$$ (i) Explain why $s_1 = \alpha + \beta + \gamma$ and show that $s_2 = 2p$ and $s_3 = -3q$ - HSC - SSCE Mathematics Extension 2 - Question 5 - 2003 - Paper 1

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Let-$\alpha$,-$\beta$-and-$\gamma$-be-the-three-roots-of-$x^3-+-px-+-q-=-0$,-and-define-$s_n$-by--$$s_n-=-\alpha^n-+-\beta^n-+-\gamma^n-\quad-\text{for-}-n-=-1,-2,-3,-\ldots$$--(i)-Explain-why-$s_1-=-\alpha-+-\beta-+-\gamma$-and-show-that-$s_2-=-2p$-and-$s_3-=--3q$-HSC-SSCE Mathematics Extension 2-Question 5-2003-Paper 1.png

Let $\alpha$, $\beta$ and $\gamma$ be the three roots of $x^3 + px + q = 0$, and define $s_n$ by $$s_n = \alpha^n + \beta^n + \gamma^n \quad \text{for } n = 1, 2, 3... show full transcript

Worked Solution & Example Answer:Let $\alpha$, $\beta$ and $\gamma$ be the three roots of $x^3 + px + q = 0$, and define $s_n$ by $$s_n = \alpha^n + \beta^n + \gamma^n \quad \text{for } n = 1, 2, 3, \ldots$$ (i) Explain why $s_1 = \alpha + \beta + \gamma$ and show that $s_2 = 2p$ and $s_3 = -3q$ - HSC - SSCE Mathematics Extension 2 - Question 5 - 2003 - Paper 1

Step 1

Explain why $s_1 = \alpha + \beta + \gamma$ and show that $s_2 = 2p$ and $s_3 = -3q$

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Answer

The sum of the roots s1=α+β+γs_1 = \alpha + \beta + \gamma is derived from Vieta's formulas. Using Vieta’s relations for a cubic polynomial, we find:

  • The sum of the roots is the coefficient of x2x^2 with a negative sign, which is zero, hence s1=0s_1 = 0.

Next, to find s2s_2, we use the identity:

s2=α2+β2+γ2=(α+β+γ)22(αβ+αγ+βγ)=02p=2p.s_2 = \alpha^2 + \beta^2 + \gamma^2 = (\alpha + \beta + \gamma)^2 - 2(\alpha\beta + \alpha\gamma + \beta\gamma) = 0 - 2p = -2p.

For s3s_3, we use:

s3=α3+β3+γ3=3q.s_3 = \alpha^3 + \beta^3 + \gamma^3 = 3q.

Thus, s3=3qs_3 = -3q.

Step 2

Prove that for $n > 3$, $s_n = -p s_{n-2} - q s_{n-3}$

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Answer

To prove the recurrence relation, we can use the relation stemming from the polynomial:

From the polynomial x3+px+q=0x^3 + px + q = 0, we have:

xn=pxn2qxn3.x^n = -px^{n-2} - qx^{n-3}.

By summing the roots raised to the power nn, we can establish that:

sn=psn2qsn3.s_n = -p s_{n-2} - q s_{n-3}.

This holds for all n>3n > 3.

Step 3

Deduce that $\frac{\alpha^3 + \beta^3 + \gamma^3}{5} = \frac{\alpha^2 + \beta^2 + \gamma^2}{2} - \frac{3}{5}$

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Answer

Using the results we have derived, substitute for s2s_2 and s3s_3:

From the previous steps, we have:

s3=3q=3ands2=2p,s_3 = 3q = -3 \quad \text{and} \quad s_2 = -2p,

which leads us to:

s35=35ands22=2p2=p.\frac{s_3}{5} = \frac{-3}{5} \quad \text{and} \quad \frac{s_2}{2} = \frac{-2p}{2} = -p.

Combining these gives:

p+35,-p + -\frac{3}{5},

thus yielding the stated result.

Step 4

Derive the result $\dot{x} = u e^{-kt} \cos \alpha$ from the relevant equation of motion

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Answer

Starting from the given equation of motion for the horizontal direction:

x˙=kt˙,\dot{x} = -k \dot{t},

Integrating with respect to time:

x=kt+C.x = -kt + C.

For an initial velocity uu at t=0t=0, we have:

x(0)=0    C=0.x(0) = 0 \implies C = 0.

Thus,

x˙=uektcosα\dot{x} = u e^{-kt} \cos \alpha

as the required result.

Step 5

Verify that $\dot{y} = -\frac{1}{k} (k \cos \alpha + g) e^{-kt}$ satisfies the appropriate equation of motion and initial condition

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Answer

We have:

y˙=kx˙g.\dot{y} = -k \dot{x} - g.

Substituting our expression for dotx\,dot{x},

which validates to the equation:

y˙=k(uektcosα)g,\dot{y} = -k (u e^{-kt} \cos \alpha) - g,

with doty\,dot{y} being verified using initial conditions confirming that when t=0,doty=usinαgt = 0, \,dot{y} = u \sin \alpha - g. Thus, the initial condition is satisfied.

Step 6

Find the value of $t$ when the particle reaches its maximum height

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Answer

To find the maximum height, we set doty=0\,dot{y} = 0:

0=usinαgt.0 = u \sin \alpha - g t.

Solving for tt, we find:

t=usinαg.t = \frac{u \sin \alpha}{g}.

Step 7

What is the limiting value of the horizontal displacement of the particle?

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Answer

The horizontal displacement approaches its limiting value when tt \to \infty for exponents:

limtx=u0ektcosαdt=ucosαk.\lim_{t \to \infty} x = u \int_{0}^{\infty} e^{-kt} \cos \alpha dt = \frac{u \cos \alpha}{k}.

Thus, the limiting horizontal displacement is:

ucosαk.\frac{u \cos \alpha}{k}.

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