The equation of the parabola is given by: \[ y = \alpha x^2 - 6x + \beta \] Since the parabola passes through the point \( (0, 2) \), substitute \( x = 0 \) and \( y = 2 \) into the equation: \[ 2 = \alpha(0)^2 - 6(0) + \beta \quad \Rightarrow \quad \beta = 2 \] Now, we need the slope of the tangent at \( x = \frac{3}{2} \) to be 0 (since the tangent is parallel to the x-axis). The derivative of the equation \( y = \alpha x^2 - 6x + \beta \) is: \[ \frac{dy}{dx} = 2\alpha x - 6 \] At \( x = \frac{3}{2} \), set the derivative equal to 0: \[ 0 = 2\alpha \left(\frac{3}{2}\right) - 6 \] Solving for \( \alpha \): \[ 0 = 3\alpha - 6 \quad \Rightarrow \quad 3\alpha = 6 \quad \Rightarrow \quad \alpha = 2 \] Therefore, the values of \( \alpha \) and \( \beta \) are \( \alpha = 2 \) and \( \beta = 2 \).
The correct answer is (C) : α = 2, β = 2.
Given the parabola \( y = \alpha x^2 - 6x + \beta \), it passes through the point (0, 2). Therefore:
\( 2 = \alpha (0)^2 - 6(0) + \beta \)
\( \beta = 2 \)
The derivative of the parabola with respect to x is:
\( \frac{dy}{dx} = 2\alpha x - 6 \)
The tangent at \( x = \frac{3}{2} \) is parallel to the x-axis, which means the slope \( \frac{dy}{dx} \) at \( x = \frac{3}{2} \) is 0:
\( 0 = 2\alpha \left( \frac{3}{2} \right) - 6 \)
\( 0 = 3\alpha - 6 \)
\( 3\alpha = 6 \)
\( \alpha = 2 \)
Therefore, \( \alpha = 2 \) and \( \beta = 2 \).
Two parabolas have the same focus $(4, 3)$ and their directrices are the $x$-axis and the $y$-axis, respectively. If these parabolas intersect at the points $A$ and $B$, then $(AB)^2$ is equal to:
A wooden block of mass M lies on a rough floor. Another wooden block of the same mass is hanging from the point O through strings as shown in the figure. To achieve equilibrium, the coefficient of static friction between the block on the floor and the floor itself is
In an experiment to determine the figure of merit of a galvanometer by half deflection method, a student constructed the following circuit. He applied a resistance of \( 520 \, \Omega \) in \( R \). When \( K_1 \) is closed and \( K_2 \) is open, the deflection observed in the galvanometer is 20 div. When \( K_1 \) is also closed and a resistance of \( 90 \, \Omega \) is removed in \( S \), the deflection becomes 13 div. The resistance of galvanometer is nearly: