We need to find the limit: \(\lim_{x \to 0} \frac{\tan x}{\sqrt{2x+4} - 2}\)
We can rationalize the denominator by multiplying by the conjugate:
\(\lim_{x \to 0} \frac{\tan x}{\sqrt{2x+4} - 2} \cdot \frac{\sqrt{2x+4} + 2}{\sqrt{2x+4} + 2}\)
\(\implies \lim_{x \to 0} \frac{\tan x (\sqrt{2x+4} + 2)}{(2x+4) - 4}\)
\(\implies \lim_{x \to 0} \frac{\tan x (\sqrt{2x+4} + 2)}{2x}\)
We can rewrite this as: \(\lim_{x \to 0} \frac{\tan x}{x} \cdot \frac{\sqrt{2x+4} + 2}{2}\)
We know that \(\lim_{x \to 0} \frac{\tan x}{x} = 1\), so we have:
\(\implies \lim_{x \to 0} 1 \cdot \frac{\sqrt{2x+4} + 2}{2}\)
Now we can substitute x = 0:
\(\implies 1 \cdot \frac{\sqrt{2(0)+4} + 2}{2}\)
\(\implies \frac{\sqrt{4} + 2}{2}\)
\(\implies \frac{2 + 2}{2}\)
\(\implies \frac{4}{2}\)
\(\implies 2\)
Therefore, the correct option is (A) 2.
The given limit is: \[ \lim_{x \to 0} \frac{\tan x}{\sqrt{2x + 4} - 2} \]
Multiply the numerator and denominator by \( \sqrt{2x + 4} + 2 \): \[ \lim_{x \to 0} \frac{\tan x}{\sqrt{2x + 4} - 2} \cdot \frac{\sqrt{2x + 4} + 2}{\sqrt{2x + 4} + 2} \] \[ \left(\sqrt{2x + 4} - 2\right) \left(\sqrt{2x + 4} + 2\right) = (2x + 4) - 4 = 2x \] \[ \lim_{x \to 0} \frac{\tan x \left( \sqrt{2x + 4} + 2 \right)}{2x} \] \( \tan x \), which is \( \tan x \approx x \) as \( x \to 0 \): \[ \lim_{x \to 0} \frac{x \left( \sqrt{2x + 4} + 2 \right)}{2x} \] The \( x \) terms cancel out: \[ \lim_{x \to 0} \frac{\sqrt{2x + 4} + 2}{2} \] \( x \to 0 \): When \( x = 0 \), we have: \[ \frac{\sqrt{2(0) + 4} + 2}{2} = \frac{\sqrt{4} + 2}{2} = \frac{2 + 2}{2} = \frac{4}{2} = 2 \]
Thus, the correct option is (A): 2
A wooden block of mass M lies on a rough floor. Another wooden block of the same mass is hanging from the point O through strings as shown in the figure. To achieve equilibrium, the coefficient of static friction between the block on the floor and the floor itself is
In an experiment to determine the figure of merit of a galvanometer by half deflection method, a student constructed the following circuit. He applied a resistance of \( 520 \, \Omega \) in \( R \). When \( K_1 \) is closed and \( K_2 \) is open, the deflection observed in the galvanometer is 20 div. When \( K_1 \) is also closed and a resistance of \( 90 \, \Omega \) is removed in \( S \), the deflection becomes 13 div. The resistance of galvanometer is nearly: