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If f(x)={tan⁡(π4−x)cot⁡2x,x≠π42K+1,x=π4f(x) = \begin{cases} \frac{\tan(\frac{\pi}{4} - x)}{\cot 2x} & , x ≠ \frac{\pi}{4} \\ 2K + 1 & , x = \frac{\pi}{4} \end{cases} is continuous at x=π4x = \frac{\pi}{4}, then the value of K is equal to

Solution

✅ Correct Option: 4

For f(x)={tan⁡(π4−x)cot⁡2x,x≠π42K+1,x=π4f(x) = \begin{cases} \frac{\tan(\frac{\pi}{4} - x)}{\cot 2x} & , x ≠ \frac{\pi}{4} \\ 2K + 1 & , x = \frac{\pi}{4} \end{cases} to be continuous at x=π4x = \frac{\pi}{4}:

lim⁡x→π4tan⁡(π4−x)cot⁡2x=2K+1\lim_{x \to \frac{\pi}{4}} \frac{\tan(\frac{\pi}{4} - x)}{\cot 2x} = 2K + 1


Substituting h=x−π4h = x - \frac{\pi}{4}:

When x→π4x \to \frac{\pi}{4}, then h→0h \to 0

π4−x=−h\frac{\pi}{4} - x = -h

x=π4+hx = \frac{\pi}{4} + h

The limit becomes:

lim⁡h→0tan⁡(−h)cot⁡(2(π4+h))\lim_{h \to 0} \frac{\tan(-h)}{\cot(2(\frac{\pi}{4} + h))}


Using tan⁡(−h)=−tan⁡h\tan(-h) = -\tan h:

cot⁡(2×π4+2h)=cot⁡(π2+2h)\cot(2 \times \frac{\pi}{4} + 2h) = \cot(\frac{\pi}{2} + 2h)

Using cot⁡(π2+θ)=−tan⁡(θ)\cot(\frac{\pi}{2} + \theta) = -\tan(\theta):

cot⁡(π2+2h)=−tan⁡(2h)\cot(\frac{\pi}{2} + 2h) = -\tan(2h)

The limit becomes:

lim⁡h→0−tan⁡h−tan⁡(2h)\lim_{h \to 0} \frac{-\tan h}{-\tan(2h)}

=lim⁡h→0tan⁡htan⁡(2h)= \lim_{h \to 0} \frac{\tan h}{\tan(2h)}


Using tan⁡(2h)=2tan⁡h1−tan⁡2h\tan(2h) = \frac{2\tan h}{1 - \tan^2 h}:

lim⁡h→0tan⁡h2tan⁡h1−tan⁡2h\lim_{h \to 0} \frac{\tan h}{\frac{2\tan h}{1 - \tan^2 h}}

=lim⁡h→0tan⁡h×(1−tan⁡2h)2tan⁡h= \lim_{h \to 0} \frac{\tan h \times (1 - \tan^2 h)}{2\tan h}

=lim⁡h→01−tan⁡2h2= \lim_{h \to 0} \frac{1 - \tan^2 h}{2}


As h→0h \to 0, tan⁡h→0\tan h \to 0:

1−022=12\frac{1 - 0^2}{2} = \frac{1}{2}


For continuity:

2K+1=122K + 1 = \frac{1}{2}

2K=12−12K = \frac{1}{2} - 1

2K=−122K = -\frac{1}{2}

K=−14K = -\frac{1}{4}

Therefore, K=−14K = -\frac{1}{4}.

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