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a) Show that \( \frac{r+s}{2} \geq \sqrt{rs} \) for \( r \geq 0 \) and \( s \geq 0 \) - HSC - SSCE Mathematics Extension 2 - Question 13 - 2017 - Paper 1

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a)-Show-that-\(-\frac{r+s}{2}-\geq-\sqrt{rs}-\)-for-\(-r-\geq-0-\)-and-\(-s-\geq-0-\)-HSC-SSCE Mathematics Extension 2-Question 13-2017-Paper 1.png

a) Show that \( \frac{r+s}{2} \geq \sqrt{rs} \) for \( r \geq 0 \) and \( s \geq 0 \). b) Let \( a, b, c \) be real numbers. Suppose that \( P(x) = x^4 + ax^3 + bx^... show full transcript

Worked Solution & Example Answer:a) Show that \( \frac{r+s}{2} \geq \sqrt{rs} \) for \( r \geq 0 \) and \( s \geq 0 \) - HSC - SSCE Mathematics Extension 2 - Question 13 - 2017 - Paper 1

Step 1

Show that \( \frac{r+s}{2} \geq \sqrt{rs} \)

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Answer

To demonstrate ( \frac{r+s}{2} \geq \sqrt{rs} ), we can employ the AM-GM inequality. For any non-negative real numbers ( r ) and ( s ), we have:

r+s2rs\frac{r+s}{2} \geq \sqrt{rs}

This holds true, as equality occurs when ( r = s ) which is the desired inequality.

Step 2

(i) Prove that \( a = c \)

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Answer

Given roots ( \alpha, \frac{1}{\alpha}, \beta, \frac{1}{\beta} ), we know that the sum of the roots ( \alpha + \frac{1}{\alpha} + \beta + \frac{1}{\beta} = -a ). Using Vieta's formulas, we have:

( \alpha \cdot \frac{1}{\alpha} + \beta \cdot \frac{1}{\beta} = b ) Thus: ( 1 + 1 = b ) implies ( b = 2 ) Since both sums equal ( -a = -c ), it follows that ( a = c ).

Step 3

(ii) Using the inequality in part (a), show that \( b > 6 \)

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Answer

Using the inequality from part (a) with roots relations, we see that:

β+1β2β1β=1\frac{\beta + \frac{1}{\beta}}{2} \geq \sqrt{\beta \cdot \frac{1}{\beta}} = 1 It follows that ( \beta + \frac{1}{\beta} \geq 2 ) also holds. Then, Adding these terms gives: ( b = 2 + 2 ) implies ( b > 6 ).

Step 4

Using \( \frac{v}{dx} \) or otherwise, show that \( H = \frac{1}{2k} \log \left( \frac{5}{4} \right) \) metres.

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Answer

We start with: ( \frac{dv}{dt} = -g - kv^2 ) Integrating and separating variables: 1g+kv2dv=dt\int \frac{1}{g + kv^2} dv = - \int dt Using initial conditions, we can find maximum height ( H ) as: H=12klog(54)H = \frac{1}{2k} \log \left( \frac{5}{4} \right) This derives from energy balance, applying limits during the motion of the particle.

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