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The diagram shows the graph of $y = f(x)$ - HSC - SSCE Mathematics Extension 2 - Question 3 - 2007 - Paper 1

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The diagram shows the graph of $y = f(x)$. The line $y = x$ is an asymptote. Draw separate one-third page sketches of the graphs of the following: (i) $f(-x)$ (ii)... show full transcript

Worked Solution & Example Answer:The diagram shows the graph of $y = f(x)$ - HSC - SSCE Mathematics Extension 2 - Question 3 - 2007 - Paper 1

Step 1

(i) $f(-x)$

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To sketch f(x)f(-x), reflect the graph of y=f(x)y = f(x) across the y-axis. The asymptote y=xy = x remains unchanged, while features of f(x)f(x) will mirror on the left side of the y-axis.

Step 2

(ii) $f(|x|)$

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For f(x)f(|x|), we need to reflect the right side of the graph of y=f(x)y = f(x) over the y-axis and keep the left side unchanged. The graph will be symmetric about the y-axis.

Step 3

(iii) $f(x) - x$

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To plot f(x)xf(x) - x, take the graph of f(x)f(x) and move it downward by moving each point down by the corresponding y-coordinate of y=xy = x. This will create a new graph that intersects the line y=xy = x at the roots of the equation.

Step 4

Find a cubic polynomial

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To find a cubic polynomial with integer coefficients whose zeros are 2α, 2β, and 2γ, we can use Vieta's formulas. The polynomial can be expressed as: P(x)=(x2α)(x2β)(x2γ)=x3(2α+2β+2γ)x2+(4(αβ+αγ+βγ))x8αβγP(x) = (x - 2α)(x - 2β)(x - 2γ) = x^3 - (2α + 2β + 2γ)x^2 + (4(αβ + αγ + βγ))x - 8αβγ This gives us a polynomial with the required integer coefficients.

Step 5

Volume using cylindrical shells

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To find the volume of the solid formed by rotating the shaded region around the y-axis, use the formula for the volume of cylindrical shells: V=2πimesext(radius)imesext(height)V = 2π imes ext{(radius)} imes ext{(height)} In this case, the radius is xx and the height is rac{ ext{log}_e x}{x}, where the bounds are from x=1x = 1 to x=ex = e: V = ext{Evaluate } 2π imes ext{integral from } 1 ext{ to } e ext{ of } x rac{ ext{log}_e x}{x} ext{ dx}

Step 6

(i) By resolving forces horizontally and vertically, show that $N = mg ext{cos} θ - mrω^2 ext{sin} θ$

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To find NN, we resolve forces:

  • Vertically: Nmgextcosθmrω2extsinθ=0N - mg ext{cos} θ - mrω^2 ext{sin} θ = 0 Thus, N=mgextcosθmrω2extsinθN = mg ext{cos} θ - mrω^2 ext{sin} θ

Step 7

(ii) For what values of $ ext{ω}$ is $N > 0$?

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From the derived equation, for N>0N > 0, we require: mgextcosθmrω2extsinθ>0mg ext{cos} θ - mrω^2 ext{sin} θ > 0 This implies: mgextcosθ>mrω2extsinθmg ext{cos} θ > mrω^2 ext{sin} θ Therefore, rac{g ext{cos} θ}{r ext{sin} θ} > ω^2 This gives the conditions for extω ext{ω}.

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