When solving limits involving trigonometric functions, use standard identities like the difference of sines identity. For limits involving \(\sin(x)\) and \(x \rightarrow 0\), recall that \( \lim\limits_{x \rightarrow 0} \frac{\sin(x)}{x} = 1 \), which simplifies many trigonometric limit problems.
The correct answer is: (B) 2, 2.
We are given the limit expression:
\( \lim\limits_{x \rightarrow 0} \frac{\sin(2+x) - \sin(2-x)}{x} \)
To solve this limit, we will use the trigonometric identity for the difference of sines:
\( \sin A - \sin B = 2 \cos\left(\frac{A+B}{2}\right) \sin\left(\frac{A-B}{2}\right) \)
Substituting \( A = 2+x \) and \( B = 2-x \), we get:
\( \sin(2+x) - \sin(2-x) = 2 \cos\left(\frac{(2+x) + (2-x)}{2}\right) \sin\left(\frac{(2+x) - (2-x)}{2}\right) \)
Simplifying further:\( = 2 \cos(2) \sin(x) \)
Now, substitute this expression back into the limit:
\( \lim\limits_{x \rightarrow 0} \frac{2 \cos(2) \sin(x)}{x} \)
Using the standard limit result \( \lim\limits_{x \rightarrow 0} \frac{\sin(x)}{x} = 1 \), we get:\( 2 \cos(2) \)
Thus, the values of \( A \) and \( B \) are 2 and 2, respectively.Therefore, the correct answer is (B) 2, 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: