The foci of the hyperbola are \( S'(4, 2) \) and \( S(8, 2) \).
The center of the hyperbola is the midpoint of the foci: \[ C = \left( \frac{4 + 8}{2}, \frac{2 + 2}{2} \right) = (6, 2) \] The distance between the foci is \( 2c = \sqrt{(8 - 4)^2 + (2 - 2)^2} = \sqrt{4^2 + 0^2} = 4 \), so \( c = 2 \).
The major axis is parallel to the x-axis since the y-coordinates of the foci are the same.
The equation of the hyperbola is of the form \( \frac{(x - h)^2}{a^2} - \frac{(y - k)^2}{b^2} = 1 \), where \( (h, k) \) is the center.
Here, \( (h, k) = (6, 2) \), so the equation is \( \frac{(x - 6)^2}{a^2} - \frac{(y - 2)^2}{b^2} = 1 \).
We have the relation \( c^2 = a^2 + b^2 \), so \( 2^2 = a^2 + b^2 \Rightarrow 4 = a^2 + b^2 \Rightarrow b^2 = 4 - a^2 \).
Since the equation involves \( y^2 \) term with a negative coefficient, we assume the given form is obtained after some manipulation of the standard equation.
Let's consider the possibility that the order of terms was swapped in the standard equation, leading to \( \frac{(y - 2)^2}{a^2} - \frac{(x - 6)^2}{b^2} = 1 \).
In this case, the major axis would be parallel to the y-axis, which contradicts the foci coordinates. So the first form is correct.
From the given equation \( 3x^2 - y^2 - \alpha x + \beta y + \gamma = 0 \), we can rewrite the standard equation:
\[ b^2 (x - 6)^2 - a^2 (y - 2)^2 = a^2 b^2 \] \[ b^2 (x^2 - 12x + 36) - a^2 (y^2 - 4y + 4) = a^2 b^2 \] \[ b^2 x^2 - a^2 y^2 - 12b^2 x + 4a^2 y + 36b^2 - 4a^2 - a^2 b^2 = 0 \]
Comparing with \( 3x^2 - y^2 - \alpha x + \beta y + \gamma = 0 \), we can assume a scaling factor \( k \): \( kb^2 = 3 \)
\( -ka^2 = -1 \Rightarrow ka^2 = 1 \) \( -12kb^2 = -\alpha \Rightarrow \alpha = 12kb^2 = 12(3) = 36 \)
\( 4ka^2 = \beta \Rightarrow \beta = 4(1) = 4 \) \( k(36b^2 - 4a^2 - a^2 b^2) = \gamma \Rightarrow 36(3) - 4(1) - (1)(3) = \gamma \Rightarrow 108 - 4 - 3 = \gamma \Rightarrow \gamma = 101 \) We have \( b^2 = 4 - a^2 \).
From \( ka^2 = 1 \) and \( kb^2 = 3 \), we get \( \frac{b^2}{a^2} = 3 \Rightarrow b^2 = 3a^2 \). So, \( 3a^2 = 4 - a^2 \Rightarrow 4a^2 = 4 \Rightarrow a^2 = 1 \).
Then \( b^2 = 3a^2 = 3(1) = 3 \). Now, \( \alpha = 36 \), \( \beta = 4 \), \( \gamma = 101 \). \( \alpha + \beta + \gamma = 36 + 4 + 101 = 141 \).
Let \( F_1, F_2 \) \(\text{ be the foci of the hyperbola}\) \[ \frac{x^2}{a^2} - \frac{y^2}{b^2} = 1, a > 0, \, b > 0, \] and let \( O \) be the origin. Let \( M \) be an arbitrary point on curve \( C \) and above the X-axis and \( H \) be a point on \( MF_1 \) such that \( MF_2 \perp F_1 F_2, \, M F_1 \perp OH, \, |OH| = \lambda |O F_2| \) with \( \lambda \in (2/5, 3/5) \), then the range of the eccentricity \( e \) is in:
Let the line $\frac{x}{4} + \frac{y}{2} = 1$ meet the x-axis and y-axis at A and B, respectively. M is the midpoint of side AB, and M' is the image of the point M across the line $x + y = 1$. Let the point P lie on the line $x + y = 1$ such that $\Delta ABP$ is an isosceles triangle with $AP = BP$. Then the distance between M' and P is:
Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is:
In the given circuit the sliding contact is pulled outwards such that the electric current in the circuit changes at the rate of 8 A/s. At an instant when R is 12 Ω, the value of the current in the circuit will be A.
For $ \alpha, \beta, \gamma \in \mathbb{R} $, if $$ \lim_{x \to 0} \frac{x^2 \sin \alpha x + (\gamma - 1)e^{x^2} - 3}{\sin 2x - \beta x} = 3, $$ then $ \beta + \gamma - \alpha $ is equal to: