The value of $\int\limits_{\frac{\pi}{3}}^{\frac{\pi}{2}} \frac{(2+3 \sin x)}{\sin x(1+\cos x)} d x$ is equal to
We start with the integral:
$\int\limits_{\frac{\pi}{3}}^{\frac{\pi}{2}} \frac{(2+3 \sin x)}{\sin x(1+\cos x)} d x$
Step 1: Simplify the integrand.
Rewrite the expression:
= 2 ∫ dx / (sinx + sinxcosx) + 3 ∫ dx / (1 + cosx)
Step 2: Solve each integral separately.
The first integral:
∫ dx / (sinx + sinxcosx) = ∫ (cosecx - cotx) cosecxc dx from π/3 to π/2
The second integral:
= ∫ (cosec x - cot x) dx = (1) from π/3 to π/2
Step 3: Combine the results.
2 * (1 - 1/√3) = 1 - 1/√3
Step 4: Solve the remaining part of the integral:
= ∫ dx / (sinx + cosx)
Use substitution and evaluate using standard methods for trigonometric integrals.
Final result:
10/3 - √3 + ln(√3)
MX is a sparingly soluble salt that follows the given solubility equilibrium at 298 K.
MX(s) $\rightleftharpoons M^{+(aq) }+ X^{-}(aq)$; $K_{sp} = 10^{-10}$
If the standard reduction potential for $M^{+}(aq) + e^{-} \rightarrow M(s)$ is $(E^{\circ}_{M^{+}/M}) = 0.79$ V, then the value of the standard reduction potential for the metal/metal insoluble salt electrode $E^{\circ}_{X^{-}/MX(s)/M}$ is ____________ mV. (nearest integer)
[Given : $\frac{2.303 RT}{F} = 0.059$ V]
An infinitely long straight wire carrying current $I$ is bent in a planar shape as shown in the diagram. The radius of the circular part is $r$. The magnetic field at the centre $O$ of the circular loop is :

There are distinct applications of integrals, out of which some are as follows:
In Maths
Integrals are used to find:
In Physics
Integrals are used to find: