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JEE Main 2019
Limits, Continuity & Differentiability
Limits, Continuity and Differentiability
Hard

Question

limx1π2sin1x1x\mathop {\lim }\limits_{x \to {1^ - }} {{\sqrt \pi - \sqrt {2{{\sin }^{ - 1}}x} } \over {\sqrt {1 - x} }} is equal to :

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Solution

1. Key Concepts and Formulas

  • Limit of a function: Understanding how to evaluate limits as a variable approaches a certain value, especially when direct substitution leads to an indeterminate form.
  • Algebraic Manipulation for Limits: Techniques like multiplying by the conjugate to simplify expressions and resolve indeterminate forms.
  • Trigonometric Identities and Standard Limits: Knowledge of inverse trigonometric identities (e.g., π2sin1x=cos1x\frac{\pi}{2} - \sin^{-1}x = \cos^{-1}x) and standard limits (e.g., limθ0sinθθ=1\mathop {\lim }\limits_{\theta \to 0} \frac{\sin \theta}{\theta} = 1).
  • Substitution in Limits: Replacing a variable with another to simplify the limit expression and change the limit point.

2. Step-by-Step Solution

The problem asks us to evaluate the limit: L=limx1π2sin1x1xL = \mathop {\lim }\limits_{x \to {1^ - }} {{\sqrt \pi - \sqrt {2{{\sin }^{ - 1}}x} } \over {\sqrt {1 - x} }}

  • Step 1: Identify the Indeterminate Form. As x1x \to 1^-, sin1xsin1(1)=π2\sin^{-1}x \to \sin^{-1}(1) = \frac{\pi}{2}. The numerator becomes π2π2=ππ=0\sqrt{\pi} - \sqrt{2 \cdot \frac{\pi}{2}} = \sqrt{\pi} - \sqrt{\pi} = 0. The denominator becomes 11=0=0\sqrt{1-1} = \sqrt{0} = 0. Thus, the limit is of the indeterminate form 00\frac{0}{0}.

  • Step 2: Rationalize the Numerator. To handle the square roots in the numerator, we multiply the numerator and denominator by the conjugate of the numerator, which is π+2sin1x\sqrt{\pi} + \sqrt{2\sin^{-1}x}. L=limx1π2sin1x1x×π+2sin1xπ+2sin1xL = \mathop {\lim }\limits_{x \to {1^ - }} {{\sqrt \pi - \sqrt {2{{\sin }^{ - 1}}x} } \over {\sqrt {1 - x} }} \times {{\sqrt \pi + \sqrt {2{{\sin }^{ - 1}}x} } \over {\sqrt \pi + \sqrt {2{{\sin }^{ - 1}}x} }} L=limx1(π)2(2sin1x)21x(π+2sin1x)L = \mathop {\lim }\limits_{x \to {1^ - }} {{(\sqrt \pi)^2 - (\sqrt {2{{\sin }^{ - 1}}x})^2 } \over {\sqrt {1 - x} \left( {\sqrt \pi + \sqrt {2{{\sin }^{ - 1}}x} } \right)}} L=limx1π2sin1x1x(π+2sin1x)L = \mathop {\lim }\limits_{x \to {1^ - }} {{\pi - 2{{\sin }^{ - 1}}x} \over {\sqrt {1 - x} \left( {\sqrt \pi + \sqrt {2{{\sin }^{ - 1}}x} } \right)}}

  • Step 3: Utilize Inverse Trigonometric Identities. We can rewrite the term π2sin1x\pi - 2\sin^{-1}x in the numerator. Recall the identity π2sin1x=cos1x\frac{\pi}{2} - \sin^{-1}x = \cos^{-1}x. So, π2sin1x=2(π2sin1x)=2cos1x\pi - 2\sin^{-1}x = 2\left(\frac{\pi}{2} - \sin^{-1}x\right) = 2\cos^{-1}x. Substituting this into the limit expression: L=limx12cos1x1x(π+2sin1x)L = \mathop {\lim }\limits_{x \to {1^ - }} {{2{{\cos }^{ - 1}}x} \over {\sqrt {1 - x} \left( {\sqrt \pi + \sqrt {2{{\sin }^{ - 1}}x} } \right)}}

  • Step 4: Separate the Limit and Evaluate Parts. We can separate the limit into parts. The term (π+2sin1x)\left( {\sqrt \pi + \sqrt {2{{\sin }^{ - 1}}x} } \right) in the denominator approaches a finite, non-zero value as x1x \to 1^-. As x1x \to 1^-, sin1xπ2\sin^{-1}x \to \frac{\pi}{2}. So, π+2sin1xπ+2π2=π+π=2π\sqrt \pi + \sqrt {2{{\sin }^{ - 1}}x} \to \sqrt \pi + \sqrt {2 \cdot \frac{\pi}{2}} = \sqrt \pi + \sqrt \pi = 2\sqrt \pi. Therefore, we can write: L=(limx12cos1x1x)×(limx11π+2sin1x)L = \left( \mathop {\lim }\limits_{x \to {1^ - }} {{2{{\cos }^{ - 1}}x} \over {\sqrt {1 - x} }} \right) \times \left( \mathop {\lim }\limits_{x \to {1^ - }} {1 \over {\sqrt \pi + \sqrt {2{{\sin }^{ - 1}}x} }} \right) L=(limx12cos1x1x)×(12π)L = \left( \mathop {\lim }\limits_{x \to {1^ - }} {{2{{\cos }^{ - 1}}x} \over {\sqrt {1 - x} }} \right) \times \left( {1 \over {2\sqrt \pi }} \right)

  • Step 5: Evaluate the Remaining Limit using Substitution. Let's focus on the limit: limx12cos1x1x\mathop {\lim }\limits_{x \to {1^ - }} {{2{{\cos }^{ - 1}}x} \over {\sqrt {1 - x} }}. We can use a substitution. Let x=cosθx = \cos \theta. As x1x \to 1^-, cosθ1\cos \theta \to 1^-. This implies θ0+\theta \to 0^+. Also, cos1x=θ\cos^{-1}x = \theta. And 1x=1cosθ\sqrt{1-x} = \sqrt{1-\cos \theta}. Using the half-angle identity 1cosθ=2sin2(θ2)1 - \cos \theta = 2\sin^2(\frac{\theta}{2}), we get 1cosθ=2sin2(θ2)=2sin(θ2)\sqrt{1-\cos \theta} = \sqrt{2\sin^2(\frac{\theta}{2})} = \sqrt{2} |\sin(\frac{\theta}{2})|. Since θ0+\theta \to 0^+, θ20+\frac{\theta}{2} \to 0^+, so sin(θ2)>0\sin(\frac{\theta}{2}) > 0. Thus, sin(θ2)=sin(θ2)|\sin(\frac{\theta}{2})| = \sin(\frac{\theta}{2}). So, 1x=2sin(θ2)\sqrt{1-x} = \sqrt{2}\sin(\frac{\theta}{2}). The limit becomes: limθ0+2θ2sin(θ2)\mathop {\lim }\limits_{\theta \to {0^+}} {{2\theta } \over {\sqrt{2}\sin \left( {{\theta \over 2}} \right)}}

  • Step 6: Apply Standard Limit Formula. We can rewrite the expression to use the standard limit limy0sinyy=1\mathop {\lim }\limits_{y \to 0} \frac{\sin y}{y} = 1. limθ0+2θ2sin(θ2)=limθ0+2θ2×1sin(θ2)\mathop {\lim }\limits_{\theta \to {0^+}} {{2\theta } \over {\sqrt{2}\sin \left( {{\theta \over 2}} \right)}} = \mathop {\lim }\limits_{\theta \to {0^+}} {{2\theta } \over {\sqrt{2}}} \times {1 \over {\sin \left( {{\theta \over 2}} \right)}} =limθ0+2θsin(θ2)= \mathop {\lim }\limits_{\theta \to {0^+}} {{\sqrt{2}\theta } \over {\sin \left( {{\theta \over 2}} \right)}} To apply the standard limit, we need θ2\frac{\theta}{2} in the denominator. =limθ0+2×θsin(θ2)=limθ0+2×2(θ2)sin(θ2)= \mathop {\lim }\limits_{\theta \to {0^+}} \sqrt{2} \times {\theta \over {\sin \left( {{\theta \over 2}} \right)}} = \mathop {\lim }\limits_{\theta \to {0^+}} \sqrt{2} \times {2 \cdot \left( {\theta \over 2} \right) \over {\sin \left( {{\theta \over 2}} \right)}} =2×2×limθ0+θ2sin(θ2)= \sqrt{2} \times 2 \times \mathop {\lim }\limits_{\theta \to {0^+}} {{\theta \over 2} \over {\sin \left( {{\theta \over 2}} \right)}} Let y=θ2y = \frac{\theta}{2}. As θ0+\theta \to 0^+, y0+y \to 0^+. =22×limy0+ysiny=22×1=22= 2\sqrt{2} \times \mathop {\lim }\limits_{y \to {0^+}} {y \over {\sin y}} = 2\sqrt{2} \times 1 = 2\sqrt{2}

  • Step 7: Combine the Results. Now, substitute the evaluated limit back into the expression for LL: L=(22)×(12π)L = (2\sqrt{2}) \times \left( {1 \over {2\sqrt \pi }} \right) L=2πL = {{\sqrt{2}} \over {\sqrt \pi }} L=2πL = \sqrt {{2 \over \pi }}

3. Common Mistakes & Tips

  • Incorrectly applying standard limits: Ensure the argument of the trigonometric function and the denominator match when using limits like limy0sinyy=1\mathop {\lim }\limits_{y \to 0} \frac{\sin y}{y} = 1.
  • Errors in trigonometric identities: Double-check identities like π2sin1x=cos1x\frac{\pi}{2} - \sin^{-1}x = \cos^{-1}x and 1cosθ=2sin2(θ2)1 - \cos \theta = 2\sin^2(\frac{\theta}{2}).
  • Substitution issues: Be careful with the direction of the limit (x1x \to 1^- implies θ0+\theta \to 0^+) and the sign of the trigonometric function after substitution (e.g., sin2(θ2)\sqrt{\sin^2(\frac{\theta}{2})}).

4. Summary

The problem involves evaluating a limit that results in an indeterminate form 00\frac{0}{0}. We began by rationalizing the numerator to simplify the expression. Next, we used the inverse trigonometric identity π2sin1x=cos1x\frac{\pi}{2} - \sin^{-1}x = \cos^{-1}x to further simplify the numerator. By separating the limit and evaluating the part with the inverse trigonometric function using a substitution (x=cosθx = \cos \theta) and a standard limit, we were able to find the value of the original limit.

The final answer is 2π\boxed{\sqrt {{2 \over \pi }}}.

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