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JEE Main 2020
Conic Sections
Hyperbola
Hard

Question

Let 0<θ<π20 < \theta < {\pi \over 2}. If the eccentricity of the hyperbola x2cos2θy2sin2θ{{{x^2}} \over {{{\cos }^2}\theta }} - {{{y^2}} \over {{{\sin }^2}\theta }} = 1 is greater than 2, then the length of its latus rectum lies in the interval :

Options

Solution

Question: Let 0<θ<π20 < \theta < {\pi \over 2}. If the eccentricity of the hyperbola x2cos2θy2sin2θ{{{x^2}} \over {{{\cos }^2}\theta }} - {{{y^2}} \over {{{\sin }^2}\theta }} = 1 is greater than 2, then the length of its latus rectum lies in the interval:

Options: (A) (3, \infty ) (B) (32,2]\left( {{3 \over 2},2} \right] (C) (1,32]\left( {1,{3 \over 2}} \right] (D) (2,3]\left( {2,3} \right]


This problem requires a strong understanding of the standard form of a hyperbola, its key parameters (eccentricity and latus rectum), and the ability to manipulate trigonometric expressions and inequalities within a specified domain. We will break down the solution into clear, logical steps, explaining the rationale behind each.


Step 1: Identify Parameters from the Standard Form of the Hyperbola

The first crucial step in any conic section problem is to correctly identify its type and extract its fundamental parameters by comparing it with the standard equation.

The given equation of the hyperbola is: x2cos2θy2sin2θ=1\frac{x^2}{\cos^2\theta} - \frac{y^2}{\sin^2\theta} = 1

We compare this with the standard form of a hyperbola centered at the origin, with its transverse axis along the x-axis: x2a2y2b2=1\frac{x^2}{a^2} - \frac{y^2}{b^2} = 1

By direct comparison, we can identify the squares of the semi-transverse axis (aa) and the semi-conjugate axis (bb): a2=cos2θa^2 = \cos^2\theta b2=sin2θb^2 = \sin^2\theta

Now, we need to find aa and bb. By definition, aa and bb represent lengths, so they must be positive values. a=cos2θ=cosθa = \sqrt{\cos^2\theta} = |\cos\theta| b=sin2θ=sinθb = \sqrt{\sin^2\theta} = |\sin\theta|

The problem statement gives us a crucial domain for θ\theta: 0<θ<π20 < \theta < \frac{\pi}{2}. In the first quadrant, both cosθ\cos\theta and sinθ\sin\theta are positive. Therefore, we can simplify: a=cosθa = \cos\theta b=sinθb = \sin\theta

Why this step is important: Correctly identifying aa and bb is foundational. An error here would propagate through all subsequent calculations. The domain 0<θ<π20 < \theta < \frac{\pi}{2} is vital for removing the absolute value signs from cos2θ\sqrt{\cos^2\theta} and sin2θ\sqrt{\sin^2\theta}.


Step 2: Calculate Eccentricity and Apply the Given Condition

The eccentricity (ee) is a characteristic parameter for a hyperbola that describes its shape, specifically how "open" its branches are. For a hyperbola of the form x2a2y2b2=1\frac{x^2}{a^2} - \frac{y^2}{b^2} = 1, the eccentricity is given by the formula: e=1+b2a2e = \sqrt{1 + \frac{b^2}{a^2}} (Alternatively, b2=a2(e21)b^2 = a^2(e^2-1) can be used, which leads to the same formula for ee.)

Now, we substitute the values of a2=cos2θa^2 = \cos^2\theta and b2=sin2θb^2 = \sin^2\theta that we found in Step 1: e=1+sin2θcos2θe = \sqrt{1 + \frac{\sin^2\theta}{\cos^2\theta}}

We recognize the fundamental trigonometric identity sin2θcos2θ=tan2θ\frac{\sin^2\theta}{\cos^2\theta} = \tan^2\theta: e=1+tan2θe = \sqrt{1 + \tan^2\theta}

Another essential trigonometric identity states that 1+tan2θ=sec2θ1 + \tan^2\theta = \sec^2\theta. Substituting this into the expression for ee: e=sec2θe = \sqrt{\sec^2\theta} e=secθe = |\sec\theta|

Again, we refer to the given domain 0<θ<π20 < \theta < \frac{\pi}{2}. In the first quadrant, cosθ\cos\theta is positive, and therefore secθ=1cosθ\sec\theta = \frac{1}{\cos\theta} is also positive. So, we can simplify secθ|\sec\theta| to secθ\sec\theta.

Thus, the eccentricity of the given hyperbola is: e=secθe = \sec\theta

The problem states that the eccentricity is greater than 2: e>2e > 2 Substituting our expression for ee: secθ>2\sec\theta > 2

Why this step is important: This step converts the problem's condition into a trigonometric inequality involving θ\theta. Mastery of trigonometric identities is crucial here. Always remember to use the absolute value when taking the square root of a squared term, and then simplify using the given domain.


Step 3: Determine the Valid Range for θ\theta

We need to solve the inequality secθ>2\sec\theta > 2 within the domain 0<θ<π20 < \theta < \frac{\pi}{2}. It's often easier to work with cosine when solving inequalities involving secant.

Recall that secθ=1cosθ\sec\theta = \frac{1}{\cos\theta}. So the inequality becomes: 1cosθ>2\frac{1}{\cos\theta} > 2

Since 0<θ<π20 < \theta < \frac{\pi}{2}, we know that cosθ\cos\theta is positive (specifically, 0<cosθ<10 < \cos\theta < 1). Because cosθ\cos\theta is positive, we can take the reciprocal of both sides of the inequality, but we must reverse the inequality sign: cosθ<12\cos\theta < \frac{1}{2}

Now, we need to find the values of θ\theta in the interval (0,π2)(0, \frac{\pi}{2}) for which cosθ<12\cos\theta < \frac{1}{2}. We know the standard value cos(π3)=12\cos\left(\frac{\pi}{3}\right) = \frac{1}{2}.

In the first quadrant (0<θ<π20 < \theta < \frac{\pi}{2}), the cosine function is a strictly decreasing function. This means that as θ\theta increases, cosθ\cos\theta decreases. Therefore, for cosθ<12\cos\theta < \frac{1}{2}, θ\theta must be greater than π3\frac{\pi}{3}.

Combining this with the initial domain 0<θ<π20 < \theta < \frac{\pi}{2}, the valid range for θ\theta that satisfies the eccentricity condition is: π3<θ<π2\frac{\pi}{3} < \theta < \frac{\pi}{2}

Why this step is important: This step establishes the critical domain for θ\theta which will be used to determine the range of the latus rectum. A common mistake is forgetting to reverse the inequality sign when taking reciprocals, or misinterpreting the monotonicity of trigonometric functions in a given quadrant. Visualizing the unit circle or the graph of cosθ\cos\theta can help avoid such errors.


Step 4: Derive the Length of the Latus Rectum

The latus rectum (LR) is a chord of the hyperbola that passes through a focus and is perpendicular to the transverse axis. Its length is another key characteristic that helps define the shape and dimensions of the hyperbola. For a hyperbola of the form x2a2y2b2=1\frac{x^2}{a^2} - \frac{y^2}{b^2} = 1, the length of the latus rectum is given by the formula: LR=2b2aLR = \frac{2b^2}{a}

Now, we substitute the values of a=cosθa = \cos\theta and b2=sin2θb^2 = \sin^2\theta that we found in Step 1: LR=2sin2θcosθLR = \frac{2\sin^2\theta}{\cos\theta}

To make it easier to analyze this expression in the next step, we can rewrite it using trigonometric identities: LR=2(sinθcosθ)sinθLR = 2 \left( \frac{\sin\theta}{\cos\theta} \right) \sin\theta LR=2tanθsinθLR = 2 \tan\theta \sin\theta

Why this step is important: This step translates the quantity we need to find (length of the latus rectum) into an expression solely in terms of θ\theta. This expression will then be analyzed over the determined range of θ\theta to find its interval.


Step 5: Find the Interval for the Length of the Latus Rectum

We need to find the range of the expression LR=2tanθsinθLR = 2 \tan\theta \sin\theta for θ\theta in the interval (π3,π2)\left( \frac{\pi}{3}, \frac{\pi}{2} \right). To do this, we will analyze the behavior of tanθ\tan\theta and sinθ\sin\theta within this specific interval.

Consider the interval (π3,π2)\left( \frac{\pi}{3}, \frac{\pi}{2} \right):

  • Behavior of tanθ\tan\theta:

    • In the first quadrant, tanθ\tan\theta is a strictly increasing function.
    • As θ\theta approaches π3\frac{\pi}{3} from the right (θπ3+\theta \to \frac{\pi}{3}^+), tanθ\tan\theta approaches tan(π3)=3\tan\left(\frac{\pi}{3}\right) = \sqrt{3}.
    • As θ\theta approaches π2\frac{\pi}{2} from the left (θπ2\theta \to \frac{\pi}{2}^-), tanθ\tan\theta approaches \infty.
    • So, tanθ(3,)\tan\theta \in (\sqrt{3}, \infty).
  • Behavior of sinθ\sin\theta:

    • In the first quadrant, sinθ\sin\theta is also a strictly increasing function.
    • As θ\theta approaches π3\frac{\pi}{3} from the right (θπ3+\theta \to \frac{\pi}{3}^+), sinθ\sin\theta approaches sin(π3)=32\sin\left(\frac{\pi}{3}\right) = \frac{\sqrt{3}}{2}.
    • As θ\theta approaches π2\frac{\pi}{2} from the left (θπ2\theta \to \frac{\pi}{2}^-), sinθ\sin\theta approaches sin(π2)=1\sin\left(\frac{\pi}{2}\right) = 1.
    • So, sinθ(32,1)\sin\theta \in \left( \frac{\sqrt{3}}{2}, 1 \right).

Since both tanθ\tan\theta and sinθ\sin\theta are positive and strictly increasing functions in the interval (π3,π2)\left( \frac{\pi}{3}, \frac{\pi}{2} \right), their product, LR=2tanθsinθLR = 2 \tan\theta \sin\theta, will also be a strictly increasing function in this interval.

Therefore, the minimum value of LRLR will be approached as θ\theta approaches π3\frac{\pi}{3} from the right, and the maximum value will be approached as θ\theta approaches π2\frac{\pi}{2} from the left.

Lower bound for LR: As θπ3+\theta \to \frac{\pi}{3}^+, LRlower_bound=2×limθπ3+(tanθ)×limθπ3+(sinθ)LR_{lower\_bound} = 2 \times \lim_{\theta \to \frac{\pi}{3}^+} (\tan\theta) \times \lim_{\theta \to \frac{\pi}{3}^+} (\sin\theta) LRlower_bound=2×tan(π3)×sin(π3)LR_{lower\_bound} = 2 \times \tan\left(\frac{\pi}{3}\right) \times \sin\left(\frac{\pi}{3}\right) LRlower_bound=2×3×32LR_{lower\_bound} = 2 \times \sqrt{3} \times \frac{\sqrt{3}}{2} LRlower_bound=2×32LR_{lower\_bound} = 2 \times \frac{3}{2} LRlower_bound=3LR_{lower\_bound} = 3 Since θ>π3\theta > \frac{\pi}{3}, this value LR=3LR=3 is not included in the interval. It defines the open lower bound.

Upper bound for LR: As θπ2\theta \to \frac{\pi}{2}^-, LRupper_bound=2×limθπ2(tanθ)×limθπ2(sinθ)LR_{upper\_bound} = 2 \times \lim_{\theta \to \frac{\pi}{2}^-} (\tan\theta) \times \lim_{\theta \to \frac{\pi}{2}^-} (\sin\theta) LRupper_bound=2×()×1LR_{upper\_bound} = 2 \times (\infty) \times 1 LRupper_bound=LR_{upper\_bound} = \infty Since θ<π2\theta < \frac{\pi}{2}, this upper bound is also not included.

Combining these results, the length of the latus rectum LRLR lies in the open interval: (3,)(3, \infty)

Why this step is important: This is the culmination of all previous steps. Analyzing the monotonicity (increasing or decreasing nature) of the function for LRLR over the derived range of θ\theta is crucial. Remember that for open intervals of θ\theta, the corresponding range of the function will also be open, meaning the endpoints are not included.


Summary and Key Takeaway:

This problem is an excellent example of how JEE questions often integrate multiple mathematical concepts. We started by correctly

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