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JEE Main 2021
Limits, Continuity & Differentiability
Limits, Continuity and Differentiability
Hard

Question

Let p=limx0+(1+tan2x)12xp = \mathop {\lim }\limits_{x \to {0^ + }} {\left( {1 + {{\tan }^2}\sqrt x } \right)^{{1 \over {2x}}}} then loglog pp is equal to :

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Solution

1. Key Concepts and Formulas

  • Limits of the form 11^\infty: When evaluating limits of the form 11^\infty, it is a standard technique to take the natural logarithm of the expression. If L=limxa[f(x)]g(x)L = \lim_{x \to a} [f(x)]^{g(x)} is of the form 11^\infty, then lnL=limxag(x)lnf(x)\ln L = \lim_{x \to a} g(x) \ln f(x).
  • Logarithm Properties: ln(ab)=blna\ln(a^b) = b \ln a.
  • Trigonometric Identities: sec2θ=1+tan2θ\sec^2 \theta = 1 + \tan^2 \theta, so ln(1+tan2x)=ln(sec2x)\ln(1 + \tan^2 \sqrt{x}) = \ln(\sec^2 \sqrt{x}).
  • L'Hôpital's Rule: If a limit of the form 00\frac{0}{0} or \frac{\infty}{\infty} is encountered, L'Hôpital's Rule can be applied: limxaf(x)g(x)=limxaf(x)g(x)\lim_{x \to a} \frac{f(x)}{g(x)} = \lim_{x \to a} \frac{f'(x)}{g'(x)}, provided the latter limit exists.
  • Standard Limit: limθ0tanθθ=1\lim_{\theta \to 0} \frac{\tan \theta}{\theta} = 1.

2. Step-by-Step Solution

We are asked to find lnp\ln p, where p=limx0+(1+tan2x)12xp = \mathop {\lim }\limits_{x \to {0^ + }} {\left( {1 + {{\tan }^2}\sqrt x } \right)^{{1 \over {2x}}}}

Step 1: Identify the indeterminate form. As x0+x \to 0^+, x0+\sqrt{x} \to 0^+. Then tanxtan0=0\tan \sqrt{x} \to \tan 0 = 0. So, 1+tan2x1+02=11 + \tan^2 \sqrt{x} \to 1 + 0^2 = 1. The exponent is 12x\frac{1}{2x}. As x0+x \to 0^+, 2x0+2x \to 0^+, so 12x+\frac{1}{2x} \to +\infty. Thus, the limit is of the indeterminate form 11^\infty.

Step 2: Take the natural logarithm of the expression. Let p=limx0+(1+tan2x)12xp = \mathop {\lim }\limits_{x \to {0^ + }} {\left( {1 + {{\tan }^2}\sqrt x } \right)^{{1 \over {2x}}}}. We will evaluate lnp\ln p: lnp=ln(limx0+(1+tan2x)12x)\ln p = \ln \left( \mathop {\lim }\limits_{x \to {0^ + }} {\left( {1 + {{\tan }^2}\sqrt x } \right)^{{1 \over {2x}}}} \right) Since the logarithm function is continuous, we can move the limit outside: lnp=limx0+ln((1+tan2x)12x)\ln p = \mathop {\lim }\limits_{x \to {0^ + }} \ln \left( {\left( {1 + {{\tan }^2}\sqrt x } \right)^{{1 \over {2x}}}} \right) Using the logarithm property ln(ab)=blna\ln(a^b) = b \ln a: lnp=limx0+12xln(1+tan2x)\ln p = \mathop {\lim }\limits_{x \to {0^ + }} \frac{1}{2x} \ln \left( {1 + {{\tan }^2}\sqrt x } \right)

Step 3: Simplify the expression inside the limit using trigonometric identities. We know the identity 1+tan2θ=sec2θ1 + \tan^2 \theta = \sec^2 \theta. Applying this with θ=x\theta = \sqrt{x}: 1+tan2x=sec2x1 + \tan^2 \sqrt{x} = \sec^2 \sqrt{x}. Substituting this into the expression for lnp\ln p: lnp=limx0+12xln(sec2x)\ln p = \mathop {\lim }\limits_{x \to {0^ + }} \frac{1}{2x} \ln \left( {\sec^2 \sqrt{x} } \right) Using the logarithm property ln(ab)=blna\ln(a^b) = b \ln a again: lnp=limx0+12x2ln(secx)\ln p = \mathop {\lim }\limits_{x \to {0^ + }} \frac{1}{2x} \cdot 2 \ln \left( {\sec \sqrt{x} } \right) lnp=limx0+1xln(secx)\ln p = \mathop {\lim }\limits_{x \to {0^ + }} \frac{1}{x} \ln \left( {\sec \sqrt{x} } \right)

Step 4: Check for indeterminate form for L'Hôpital's Rule. As x0+x \to 0^+, x0+\sqrt{x} \to 0^+, and secxsec0=1\sec \sqrt{x} \to \sec 0 = 1. So, ln(secx)ln(1)=0\ln(\sec \sqrt{x}) \to \ln(1) = 0. The denominator is xx, which also approaches 00. Thus, the limit is now of the indeterminate form 00\frac{0}{0}, and we can apply L'Hôpital's Rule.

Step 5: Apply L'Hôpital's Rule. Let f(x)=ln(secx)f(x) = \ln(\sec \sqrt{x}) and g(x)=xg(x) = x. We need to find the derivatives f(x)f'(x) and g(x)g'(x). g(x)=ddx(x)=1g'(x) = \frac{d}{dx}(x) = 1. To find f(x)f'(x), we use the chain rule: f(x)=ddx[ln(secx)]f'(x) = \frac{d}{dx} [\ln(\sec \sqrt{x})] Let u=secxu = \sec \sqrt{x}. Then dfdx=ddu(lnu)dudx=1ududx\frac{df}{dx} = \frac{d}{du}(\ln u) \cdot \frac{du}{dx} = \frac{1}{u} \cdot \frac{du}{dx}. Now, we find dudx\frac{du}{dx}: dudx=ddx(secx)\frac{du}{dx} = \frac{d}{dx} (\sec \sqrt{x}) Let v=xv = \sqrt{x}. Then dudx=ddv(secv)dvdx=(secvtanv)dvdx\frac{du}{dx} = \frac{d}{dv}(\sec v) \cdot \frac{dv}{dx} = (\sec v \tan v) \cdot \frac{dv}{dx}. dvdx=ddx(x1/2)=12x1/2=12x\frac{dv}{dx} = \frac{d}{dx} (x^{1/2}) = \frac{1}{2} x^{-1/2} = \frac{1}{2\sqrt{x}}. So, dudx=secxtanx12x\frac{du}{dx} = \sec \sqrt{x} \tan \sqrt{x} \cdot \frac{1}{2\sqrt{x}}. Substituting back into f(x)f'(x): f(x)=1secx(secxtanx12x)f'(x) = \frac{1}{\sec \sqrt{x}} \cdot \left( \sec \sqrt{x} \tan \sqrt{x} \cdot \frac{1}{2\sqrt{x}} \right) f(x)=tanx2xf'(x) = \frac{\tan \sqrt{x}}{2\sqrt{x}}.

Applying L'Hôpital's Rule: lnp=limx0+f(x)g(x)=limx0+tanx2x1\ln p = \mathop {\lim }\limits_{x \to {0^ + }} \frac{f'(x)}{g'(x)} = \mathop {\lim }\limits_{x \to {0^ + }} \frac{\frac{\tan \sqrt{x}}{2\sqrt{x}}}{1} lnp=limx0+tanx2x\ln p = \mathop {\lim }\limits_{x \to {0^ + }} \frac{\tan \sqrt{x}}{2\sqrt{x}}

Step 6: Evaluate the resulting limit. We can rewrite the limit as: lnp=12limx0+tanxx\ln p = \frac{1}{2} \mathop {\lim }\limits_{x \to {0^ + }} \frac{\tan \sqrt{x}}{\sqrt{x}} Let y=xy = \sqrt{x}. As x0+x \to 0^+, y0+y \to 0^+. The limit becomes: lnp=12limy0+tanyy\ln p = \frac{1}{2} \mathop {\lim }\limits_{y \to 0^ + } \frac{\tan y}{y} We know the standard limit limy0tanyy=1\mathop {\lim }\limits_{y \to 0} \frac{\tan y}{y} = 1. Therefore, lnp=121=12\ln p = \frac{1}{2} \cdot 1 = \frac{1}{2}

3. Common Mistakes & Tips

  • Incorrectly applying L'Hôpital's Rule: Ensure the limit is indeed in an indeterminate form (00\frac{0}{0} or \frac{\infty}{\infty}) before applying the rule. Also, be careful with the differentiation of composite functions, especially involving square roots and trigonometric functions.
  • Algebraic Errors: Mistakes in simplifying trigonometric expressions or applying logarithm properties can lead to incorrect results. Double-check these steps.
  • Ignoring the 11^\infty form: If a limit is of the form 11^\infty, directly substituting values will not work. Always convert it to the form elimg(x)lnf(x)e^{\lim g(x)\ln f(x)} or take the logarithm as shown here.

4. Summary

The problem involves evaluating a limit of the indeterminate form 11^\infty. We began by taking the natural logarithm of the given expression for pp, transforming the limit into a form where L'Hôpital's Rule could be applied. After simplifying the expression using trigonometric identities and logarithm properties, we applied L'Hôpital's Rule to differentiate the numerator and denominator. The resulting limit simplified to a standard trigonometric limit, allowing us to find the value of lnp\ln p.

The value of lnp\ln p was found to be 12\frac{1}{2}.

The final answer is \boxed{{1 \over 2}}.

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