Using partial fractions, we can write \[ \frac{6}{(e^x + 1)(e^x + 2)(e^x + 3)} = \frac{A}{e^x + 1} + \frac{B}{e^x + 2} + \frac{C}{e^x + 3}. \] Solving for \(A, B, C\) gives \[ A = \tfrac{1}{2}, \quad B = -1, \quad C = \tfrac{1}{2}. \] Hence \[ \frac{6}{(e^x + 1)(e^x + 2)(e^x + 3)} = \frac{1/2}{e^x + 1} - \frac{1}{e^x + 2} + \frac{1/2}{e^x + 3}. \] Therefore the integral becomes \[ I = \int_{0}^{\infty} \frac{6}{(e^x + 1)(e^x + 2)(e^x + 3)} \, dx = \int_{0}^{\infty} \left(\frac{1/2}{e^x + 1} - \frac{1}{e^x + 2} + \frac{1/2}{e^x + 3}\right) \, dx. \] Each term can be integrated via the substitution \(u = e^x\), \(du = e^x \, dx\). Carrying out these integrals and evaluating from \(x=0\) to \(x \to \infty\) yields \[ I = \ln\left(\tfrac{32}{27}\right). \] \[ \boxed{ \int_{0}^{\infty} \frac{6}{(e^x + 1)(e^x + 2)(e^x + 3)} \, dx = \ln\left(\tfrac{32}{27}\right). } \]
Let \( f : (0, \infty) \to \mathbb{R} \) be a twice differentiable function. If for some \( a \neq 0 \), } \[ \int_0^a f(x) \, dx = f(a), \quad f(1) = 1, \quad f(16) = \frac{1}{8}, \quad \text{then } 16 - f^{-1}\left( \frac{1}{16} \right) \text{ is equal to:}\]

Two circular discs of radius \(10\) cm each are joined at their centres by a rod, as shown in the figure. The length of the rod is \(30\) cm and its mass is \(600\) g. The mass of each disc is also \(600\) g. If the applied torque between the two discs is \(43\times10^{-7}\) dyne·cm, then the angular acceleration of the system about the given axis \(AB\) is ________ rad s\(^{-2}\).

The representation of the area of a region under a curve is called to be as integral. The actual value of an integral can be acquired (approximately) by drawing rectangles.
Also, F(x) is known to be a Newton-Leibnitz integral or antiderivative or primitive of a function f(x) on an interval I.
F'(x) = f(x)
For every value of x = I.
Integral calculus helps to resolve two major types of problems: