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if `theta and phi` are eccentric angles of the ends of a pair of conjugate diameters of the ellipse `(x^(2))/(a^(2))+(y^(2))/(b^(2))=1` then `( theta - phi)` is equal to

A

`+- pi //2`

B

`+- pi`

C

0

D

none of these

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To solve the problem, we need to find the value of \( \theta - \phi \) where \( \theta \) and \( \phi \) are the eccentric angles of the ends of a pair of conjugate diameters of the ellipse given by the equation: \[ \frac{x^2}{a^2} + \frac{y^2}{b^2} = 1 \] ### Step 1: Understanding the Eccentric Angles The eccentric angles \( \theta \) and \( \phi \) correspond to points on the ellipse. For any point on the ellipse, the coordinates can be expressed in terms of the eccentric angle \( \theta \) as: \[ x = a \cos \theta, \quad y = b \sin \theta \] ### Step 2: Equations of the Conjugate Diameters The equations of the conjugate diameters can be expressed using the tangent equations corresponding to \( \theta \) and \( \phi \): 1. For angle \( \theta \): \[ \frac{x}{a} \cos \theta + \frac{y}{b} \sin \theta = 1 \] 2. For angle \( \phi \): \[ \frac{x}{a} \cos \phi + \frac{y}{b} \sin \phi = 1 \] ### Step 3: Finding the Slopes of the Diameters From the tangent equations, we can derive the slopes of the lines corresponding to \( \theta \) and \( \phi \): - The slope \( m_1 \) corresponding to \( \theta \): \[ m_1 = -\frac{b \cos \theta}{a \sin \theta} \] - The slope \( m_2 \) corresponding to \( \phi \): \[ m_2 = -\frac{b \cos \phi}{a \sin \phi} \] ### Step 4: Condition for Conjugate Diameters For conjugate diameters, the product of their slopes should satisfy: \[ m_1 \cdot m_2 = -\frac{b^2}{a^2} \] Substituting the expressions for \( m_1 \) and \( m_2 \): \[ \left(-\frac{b \cos \theta}{a \sin \theta}\right) \left(-\frac{b \cos \phi}{a \sin \phi}\right) = -\frac{b^2}{a^2} \] This simplifies to: \[ \frac{b^2 \cos \theta \cos \phi}{a^2 \sin \theta \sin \phi} = -\frac{b^2}{a^2} \] ### Step 5: Simplifying the Equation Cancelling \( \frac{b^2}{a^2} \) from both sides gives: \[ \frac{\cos \theta \cos \phi}{\sin \theta \sin \phi} = -1 \] This can be rewritten as: \[ \cot \theta \cot \phi = -1 \] ### Step 6: Solving for \( \theta - \phi \) From the equation \( \cot \theta \cot \phi = -1 \), we can conclude: \[ \cot \theta = -\cot \phi \] This implies: \[ \theta = 90^\circ + \phi \quad \text{or} \quad \theta = \frac{\pi}{2} + \phi \quad (\text{in radians}) \] ### Step 7: Final Result Thus, we find: \[ \theta - \phi = \frac{\pi}{2} \] ### Conclusion The value of \( \theta - \phi \) is: \[ \theta - \phi = \frac{\pi}{2} \]
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