Right-hand limit (RHL): As \( x \to 0^+ \), using the first case yields \[ \lim\limits_{h \to 0^+} \frac{\tan^2 h}{h^2} = 1 \].
- Left-hand limit (LHL): As \( x \to 0^- \), using the third case results in \[ \lim\limits_{h \to 0^-} \sqrt{(-h) \cot(-h)} \]. Applying \( \cot(-h) = -\cot h \), we obtain \[ \lim\limits_{h \to 0^-} \sqrt{(1-h) \cot(1-h)} \]. This value is not equal to \( \lim\limits_{x \to 0^+} f(x) \), therefore, \[ \lim\limits_{x \to 0} f(x) { does not exist}. \]
\(\lim_{{x \to 0}} \limits\) \(\frac{cos(sin x) - cos x }{x^4}\) is equal to :