When solving integrals involving trigonometric functions, consider using substitutions to simplify the expression. Using the substitution \( t = \tan x \) often helps transform the integral into a simpler form, as shown in this example.
The correct answer is: (A): \(\frac{1}{6}\tan^{-1}\left(\frac{2\tan x}{3}\right) + C\)
We are tasked with evaluating the integral:
\(\int \frac{1}{1 + 3\sin^2 x + 8 \cos^2 x} \, dx\)
Step 1: Simplify the expression
The given expression contains both sine and cosine terms. We begin by rewriting the denominator to combine like terms:
\( 1 + 3\sin^2 x + 8\cos^2 x = 1 + 3\sin^2 x + 8(1 - \sin^2 x) = 1 + 3\sin^2 x + 8 - 8\sin^2 x \)
After simplifying, we get:
\( 9 - 5\sin^2 x \)
Step 2: Use a substitution to simplify further
Next, we use the substitution \( t = \tan x \), which implies that \( \sec^2 x \, dx = dt \). Since \( \sin^2 x = \frac{t^2}{1 + t^2} \), we can rewrite the denominator in terms of \( t \). The integral becomes:
\( \int \frac{1}{9 - 5\frac{t^2}{1 + t^2}} \, dt \)
Step 3: Simplify the expression
After simplifying the denominator, we get a rational function of \( t \), which can be integrated using standard methods. The resulting integral simplifies to:
\( \frac{1}{6}\tan^{-1}\left(\frac{2t}{3}\right) + C \)
Step 4: Substitute back to original variable
Finally, substitute \( t = \tan x \) back into the expression to get the final result:
\( \frac{1}{6}\tan^{-1}\left(\frac{2\tan x}{3}\right) + C \)
Conclusion:
The correct answer is (A): \(\frac{1}{6}\tan^{-1}\left(\frac{2\tan x}{3}\right) + C\)
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:
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