a)
\[ f(2) = 0\]
b) To find it, we need to use the property that the domain of the initial function is the range of the inverse, and vice versa. So:
\[ f(0) = 8\]
\[ f^{-1}(8) = 0\]
c) This will be a reflection in the y-axis.
a) To obtain \( h(x) = 3(x+2)^2 \) from \( g(x) = x^2 \), the following geometric transformations are applied:
b) We have to follow the transformations outlined in part (a):
Therefore, the coordinates of \( Q \) are \( (0, 12) \).
Closea) (i), (ii), (iii) The transformations given for \( g(x) = \frac{1}{2}(f(x-2)) + 3 \) allow us to identify the coefficients:
So, \( a = 2 \), \( b = 3 \), and \( c = \frac{1}{2} \).
b) To find the coordinates of point \( B \) on \( h(x) = 4g(x) - 2 \), we apply the following steps:
Therefore, the coordinates of point \( B \) are \( (1, 12) \).
Closea) (i), (ii), (iii) To find the values of \( p \), \( q \), and \( r \) for \( g(x) = p(x+q)^3 + r \), we apply the given transformations to \( f(x) = 5x^3 + 25 \):
b) To find \( g'(x) \), we differentiate \( g(x) = \frac{5}{2}(x-2)^3 + 3 \):
\[ g'(x) = \frac{5}{2} \times 3(x-2)^2 = \frac{15}{2}(x-2)^2 \]
c) The function \( g(x) \) is increasing where \( g'(x) > 0 \). Since \( g'(x) = \frac{15}{2}(x-2)^2 \), which is always non-negative, \( g(x) \) is increasing for all \( x \in \mathbb{R} \).
Closea)
\[ f(1) = (1)^2 + 2(1) - 8 = 1 + 2 - 8 = -5 \]
b) Finding the factors of \(-8\) that add up to \(2\) yields \(4\) and \(-2\).
\[ f(x) = (x + 4)(x - 2) \]
Thus, \( a = 4 \) and \( b = 2 \).
c) To find the distance traveled by the particle from \( x = 3 \) to \( x = 6 \), we calculate the integral:
\[ \text{Distance} = \int_{3}^{6} |x^2 + 2x - 8| \, dx = 66 \]
This can be easily found in the GDC:
d) Reflecting in the y-axis:
\[ f(-x) = (-x)^2 + 2(-x) - 8 = x^2 - 2x - 8 \]
Translate 2 units to the left: \[ g(x) = (x + 2)^2 - 2(x + 2) - 8 \]
\[ = x^2 + 4x + 4 - 2x - 4 - 8 \]
\[ = x^2 + 2x - 8 \]
Closea)
Horizontal Translation: The term \( x + \pi \) indicates a horizontal shift by \(-\pi\) units. This translates the function to the left by \(\pi\) units.
Vertical Translation: The change from \( a \) to \( b \) shows a vertical shift. Since \( b \) is less than \( a \), the function is shifted downwards by \( a - b \) units.
b) (i) & (ii) Point \( A(0, 4) \) is on \( f(x) \), so:
\[ f(0) = 2\sin(0) + a = a \] We need to find \( a \) such that when \( x = 0 \), \( f(x) = 4 \). Hence, \( a = 4 \).
Point \( B(\pi, 2) \) is on \( g(x) \), so: \[ g(\pi) = 2\sin(\pi + \pi) + b = 2\sin(2\pi) + b = b \] Since \( g(\pi) = 2 \), we have \( b = 2 \).
c) The function \( g(x) = 2\sin(x + \pi) + b \) has the same amplitude and period as \( f(x) \), but with a vertical shift. The range of \( \sin(x) \) is \([-1, 1]\), so the range of \( 2\sin(x) \) is \([-2, 2]\). Adding \( b = 2 \), the range of \( g(x) \) is:
\[ [-2 + 2, 2 + 2] = [0, 4] \]
Closea) To find \( a \), we use the axis of symmetry formula for a quadratic function \( f(x) = 3x^2 + ax - 18 \). The axis of symmetry is given by:
\[ x = -\frac{b}{2a} \]
For the function \( f(x) = 3x^2 + ax - 18 \), the axis of symmetry is \( \frac{1}{2} \). Thus:
\[ \frac{1}{2} = -\frac{a}{2 \times 3} \]
Solving for \( a \):
\[ \frac{1}{2} = -\frac{a}{6} \]
\[ a = -3 \]
b) Substitute \( x = \frac{1}{2} \) into \( f(x) \):
\[ f\left(\frac{1}{2}\right) = 3\left(\frac{1}{2}\right)^2 - 3\left(\frac{1}{2}\right) - 18 \]
\[ = 3 \cdot \frac{1}{4} - \frac{3}{2} - 18 = \frac{3}{4} - \frac{3}{2} - 18 = -\frac{63}{4} \]
Thus, the vertex is: \(\left(\frac{1}{2}, -\frac{63}{4}\right)\)
c) To find the exact roots of the function, we solve:
\[ 3x^2 - 3x - 18 = 0 \]
\[ x^2 - x - 6 = 0 \]
\[ (x-3)(x+2) = 0 \]
\[ x = 3, \ x = -2 \]
d) Point \( M(1, -18) \) on \( f(x) \) is reflected across the x-axis to get \( N \) on \( g(x) \). The reflection changes the y-coordinate sign and doesn't affect the x-coordinate:
\[ N(1, 18) \]
Closea) (i) & (ii) Vertical asymptote occurs where the denominator of the fraction equals zero, which makes the function undefined:
\[ x + 1 = 0 \]
\[ x = -1 \]
As \( x \) approaches infinity, the term \(\frac{2}{x+1}\) approaches zero. Thus, the function approaches:
\[ f(x) \to 2 - 0 = 2 \]
The horizontal asymptote is: \( y = 2 \)
b) (i) Set \( f(x) = 0 \):
\[ 2 - \frac{2}{x+1} = 0 \]
\[ \frac{2}{x+1} = 2 \]
\[ 2 = 2(x + 1) \]
\[ 2 = 2x + 2 \]
\[ 0 = 2x \]
\[ x = 0 \]
The x-intercept is: \( (0, 0) \)
b) (ii) Set \( x=0 \):
\[ f(0) = 2 - \frac{2}{0+1} \]
\[ f(0) = 2 - 2 = 0 \]
The y-intercept is: \( (0, 0) \)
c) Let's start with the reflection in the y-axis. Replace \( x \) with \( -x \) in \( f(x) \):
\[ f(-x) = 2 - \frac{2}{-x + 1} \]
\[ = 2 + \frac{2}{x - 1} \]
For the horizontal stretch of 3 we replace \( x \) with \( \frac{x}{3} \):
\[ g(x) = 2 + \frac{2}{\frac{x}{3} - 1} \]
\[ g(x) = 2 + \frac{2}{\frac{x - 3}{3}} \]
\[ g(x) = 2 + \frac{6}{x - 3} \]
Close