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JEE Main 2024
Limits, Continuity & Differentiability
Limits, Continuity and Differentiability
Hard

Question

If the function f(x) = \left\{ {\matrix{ {(1 + |\cos x|)^{\lambda \over {|\cos x|}}} & , & {0 < x < {\pi \over 2}} \cr \mu & , & {x = {\pi \over 2}} \cr e^{{{\cot 6x} \over {{}\cot 4x}}} & , & {{\pi \over 2} < x < \pi } \cr } } \right. is continuous at x=π2x = {\pi \over 2}, then 9λ+6logeμ+μ6e6λ9\lambda + 6{\log _e}\mu + {\mu ^6} - {e^{6\lambda }} is equal to

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Solution

1. Key Concepts and Formulas

  • Continuity of a Function: A function f(x)f(x) is continuous at a point x=cx=c if the following three conditions are met:
    • f(c)f(c) is defined.
    • limxcf(x)\mathop {\lim }\limits_{x \rightarrow c} f(x) exists.
    • limxcf(x)=f(c)\mathop {\lim }\limits_{x \rightarrow c} f(x) = f(c). For a piecewise function, this implies that the left-hand limit, the right-hand limit, and the function value at the point must all be equal.
    • Left-hand limit: limxcf(x)\mathop {\lim }\limits_{x \rightarrow c^-} f(x)
    • Right-hand limit: limxc+f(x)\mathop {\lim }\limits_{x \rightarrow c^+} f(x)
    • Function value: f(c)f(c)
  • Limit of the form (1+u)1/u(1+u)^{1/u}: A standard limit form is limu0(1+u)1/u=e\mathop {\lim }\limits_{u \rightarrow 0} (1+u)^{1/u} = e. This can be generalized to limu0(1+u)k/u=ek\mathop {\lim }\limits_{u \rightarrow 0} (1+u)^{k/u} = e^k.
  • Trigonometric Identities and Limits:
    • cotx=cosxsinx\cot x = \frac{\cos x}{\sin x}
    • limx0sin(ax)bx=ab\lim_{x \to 0} \frac{\sin(ax)}{bx} = \frac{a}{b} and limx0tan(ax)bx=ab\lim_{x \to 0} \frac{\tan(ax)}{bx} = \frac{a}{b}.
    • When dealing with limits of trigonometric functions as xπ/2x \to \pi/2, it's often helpful to consider the substitution x=π/2+hx = \pi/2 + h or x=π/2hx = \pi/2 - h and use small angle approximations or standard limits.

2. Step-by-Step Solution

Step 1: Evaluate the left-hand limit at x=π2x = \frac{\pi}{2}. For 0<x<π20 < x < \frac{\pi}{2}, the function is given by f(x)=(1+cosx)λcosxf(x) = (1 + |\cos x|)^{\frac{\lambda}{|\cos x|}}. As xπ2x \to \frac{\pi}{2}^-, xx approaches π2\frac{\pi}{2} from values less than π2\frac{\pi}{2}. In this interval, cosx>0\cos x > 0, so cosx=cosx|\cos x| = \cos x. Let u=cosxu = \cos x. As xπ2x \to \frac{\pi}{2}^-, u=cosxcos(π2)=0u = \cos x \to \cos(\frac{\pi}{2}) = 0. The left-hand limit becomes: limxπ2(1+cosx)λcosx=limu0+(1+u)λu\mathop {\lim }\limits_{x \rightarrow \frac{\pi^{-}}{2}} (1 + |\cos x|)^{\frac{\lambda}{|\cos x|}} = \mathop {\lim }\limits_{u \rightarrow 0^+} (1+u)^{\frac{\lambda}{u}} Using the standard limit form limu0(1+u)k/u=ek\mathop {\lim }\limits_{u \rightarrow 0} (1+u)^{k/u} = e^k, we get: limu0+(1+u)λu=eλ\mathop {\lim }\limits_{u \rightarrow 0^+} (1+u)^{\frac{\lambda}{u}} = e^\lambda Thus, the left-hand limit is eλe^\lambda.

Step 2: Evaluate the right-hand limit at x=π2x = \frac{\pi}{2}. For π2<x<π\frac{\pi}{2} < x < \pi, the function is given by f(x)=ecot6xcot4xf(x) = e^{\frac{\cot 6x}{\cot 4x}}. As xπ2+x \to \frac{\pi}{2}^+, xx approaches π2\frac{\pi}{2} from values greater than π2\frac{\pi}{2}. We need to evaluate: limxπ+2ecot6xcot4x\mathop {\lim }\limits_{x \rightarrow \frac{\pi^{+}}{2}} e^{\frac{\cot 6x}{\cot 4x}} Let's first evaluate the exponent: limxπ+2cot6xcot4x\mathop {\lim }\limits_{x \rightarrow \frac{\pi^{+}}{2}} \frac{\cot 6x}{\cot 4x}. We can write cotx=cosxsinx\cot x = \frac{\cos x}{\sin x}. So the limit is: limxπ+2cos6xsin6xsin4xcos4x\mathop {\lim }\limits_{x \rightarrow \frac{\pi^{+}}{2}} \frac{\cos 6x}{\sin 6x} \cdot \frac{\sin 4x}{\cos 4x} As xπ2+x \to \frac{\pi}{2}^+, let x=π2+hx = \frac{\pi}{2} + h, where h0+h \to 0^+. Then: 6x=6(π2+h)=3π+6h6x = 6(\frac{\pi}{2} + h) = 3\pi + 6h 4x=4(π2+h)=2π+4h4x = 4(\frac{\pi}{2} + h) = 2\pi + 4h

cos(6x)=cos(3π+6h)=cos(π+6h)=cos(6h)\cos(6x) = \cos(3\pi + 6h) = \cos(\pi + 6h) = -\cos(6h) sin(6x)=sin(3π+6h)=sin(π+6h)=sin(6h)\sin(6x) = \sin(3\pi + 6h) = \sin(\pi + 6h) = -\sin(6h) cos(4x)=cos(2π+4h)=cos(4h)\cos(4x) = \cos(2\pi + 4h) = \cos(4h) sin(4x)=sin(2π+4h)=sin(4h)\sin(4x) = \sin(2\pi + 4h) = \sin(4h)

The exponent limit becomes: limh0+cos6hsin6hsin4hcos4h=limh0+cos6hsin6hsin4hcos4h\mathop {\lim }\limits_{h \rightarrow 0^+} \frac{-\cos 6h}{-\sin 6h} \cdot \frac{\sin 4h}{\cos 4h} = \mathop {\lim }\limits_{h \rightarrow 0^+} \frac{\cos 6h}{\sin 6h} \cdot \frac{\sin 4h}{\cos 4h} We can rewrite this as: limh0+(cos6hcos4h)(sin4h1)(1sin6h)\mathop {\lim }\limits_{h \rightarrow 0^+} \left( \frac{\cos 6h}{\cos 4h} \right) \cdot \left( \frac{\sin 4h}{1} \right) \cdot \left( \frac{1}{\sin 6h} \right) =limh0+(cos6hcos4h)(sin4h4h4h)(6hsin6h16h)= \mathop {\lim }\limits_{h \rightarrow 0^+} \left( \frac{\cos 6h}{\cos 4h} \right) \cdot \left( \frac{\sin 4h}{4h} \cdot 4h \right) \cdot \left( \frac{6h}{\sin 6h} \cdot \frac{1}{6h} \right) =limh0+(cos6hcos4h)(sin4h4h)(6hsin6h)4h6h= \mathop {\lim }\limits_{h \rightarrow 0^+} \left( \frac{\cos 6h}{\cos 4h} \right) \cdot \left( \frac{\sin 4h}{4h} \right) \cdot \left( \frac{6h}{\sin 6h} \right) \cdot \frac{4h}{6h} As h0h \to 0: cos6hcos0=1\cos 6h \to \cos 0 = 1 cos4hcos0=1\cos 4h \to \cos 0 = 1 sin4h4h1\frac{\sin 4h}{4h} \to 1 6hsin6h1\frac{6h}{\sin 6h} \to 1 4h6h=23\frac{4h}{6h} = \frac{2}{3}

So, the limit of the exponent is: (1/1)1123=23(1/1) \cdot 1 \cdot 1 \cdot \frac{2}{3} = \frac{2}{3} Therefore, the right-hand limit is e2/3e^{2/3}.

Step 3: Evaluate the function value at x=π2x = \frac{\pi}{2}. At x=π2x = \frac{\pi}{2}, the function is defined as f(π2)=μf(\frac{\pi}{2}) = \mu.

Step 4: Apply the continuity condition. For the function to be continuous at x=π2x = \frac{\pi}{2}, the left-hand limit, the right-hand limit, and the function value must be equal: limxπ2f(x)=limxπ+2f(x)=f(π2)\mathop {\lim }\limits_{x \rightarrow \frac{\pi^{-}}{2}} f(x) = \mathop {\lim }\limits_{x \rightarrow \frac{\pi^{+}}{2}} f(x) = f(\frac{\pi}{2}) eλ=e2/3=μe^\lambda = e^{2/3} = \mu From this equality, we can determine the values of λ\lambda and μ\mu: λ=23\lambda = \frac{2}{3} μ=e2/3\mu = e^{2/3}

Step 5: Calculate the required expression. We need to find the value of 9λ+6logeμ+μ6e6λ9\lambda + 6\log_e\mu + \mu^6 - e^{6\lambda}. Substitute the values of λ\lambda and μ\mu: 9λ=9×23=69\lambda = 9 \times \frac{2}{3} = 6 6logeμ=6loge(e2/3)=6×23=46\log_e\mu = 6\log_e(e^{2/3}) = 6 \times \frac{2}{3} = 4 μ6=(e2/3)6=e(2/3)×6=e4\mu^6 = (e^{2/3})^6 = e^{(2/3) \times 6} = e^4 e6λ=e6×(2/3)=e12/3=e4e^{6\lambda} = e^{6 \times (2/3)} = e^{12/3} = e^4

Now, substitute these values into the expression: 9λ+6logeμ+μ6e6λ=6+4+e4e49\lambda + 6\log_e\mu + \mu^6 - e^{6\lambda} = 6 + 4 + e^4 - e^4 =10= 10

3. Common Mistakes & Tips

  • Sign errors with trigonometric functions: Be careful with the signs of trigonometric functions in different quadrants. For xπ2x \to \frac{\pi}{2}^-, cosx>0\cos x > 0, and for xπ2+x \to \frac{\pi}{2}^+, cosx<0\cos x < 0. However, in the first part of the limit, cosx|\cos x| simplifies to cosx\cos x as xπ2x \to \frac{\pi}{2}^-.
  • Handling indeterminate forms: Limits of the form elimit of exponente^{\text{limit of exponent}} are common. Ensure the limit of the exponent is correctly evaluated, especially for trigonometric functions. Using substitutions like x=π2+hx = \frac{\pi}{2} + h can simplify the evaluation of limits as xπ2x \to \frac{\pi}{2}.
  • Algebraic manipulation of limits: When evaluating limits involving trigonometric functions like cot6xcot4x\frac{\cot 6x}{\cot 4x}, rewriting them in terms of sin\sin and cos\cos and then using standard limits like limy0sin(ay)by=ab\lim_{y \to 0} \frac{\sin(ay)}{by} = \frac{a}{b} is a robust strategy.

4. Summary

The problem requires us to find the value of an expression involving λ\lambda and μ\mu by ensuring the continuity of a piecewise function at x=π2x = \frac{\pi}{2}. We first evaluated the left-hand limit as xx approaches π2\frac{\pi}{2} from the left, which resulted in eλe^\lambda. Next, we computed the right-hand limit as xx approaches π2\frac{\pi}{2} from the right, which involved evaluating a limit of the form eexponente^{\text{exponent}} and found the exponent's limit to be 23\frac{2}{3}, leading to a right-hand limit of e2/3e^{2/3}. The function value at x=π2x = \frac{\pi}{2} is given as μ\mu. By equating these three values for continuity, we determined λ=23\lambda = \frac{2}{3} and μ=e2/3\mu = e^{2/3}. Finally, we substituted these values into the given expression 9λ+6logeμ+μ6e6λ9\lambda + 6\log_e\mu + \mu^6 - e^{6\lambda}, simplifying it to 6+4+e4e4=106 + 4 + e^4 - e^4 = 10.

5. Final Answer

The final answer is 10\boxed{10}.

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