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 \[ I = \ln\left(\tfrac{32}{27}\right). \] \[ \boxed{ \int_{0}^{\infty} \frac{6}{(e^x + 1)(e^x + 2)(e^x + 3)} \, dx = \ln\left(\tfrac{32}{27}\right). } \]
In the given circuit the sliding contact is pulled outwards such that the electric current in the circuit changes at the rate of 8 A/s. At an instant when R is 12 Ω, the value of the current in the circuit will be A.
Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is:
For $ \alpha, \beta, \gamma \in \mathbb{R} $, if $$ \lim_{x \to 0} \frac{x^2 \sin \alpha x + (\gamma - 1)e^{x^2} - 3}{\sin 2x - \beta x} = 3, $$ then $ \beta + \gamma - \alpha $ is equal to:
The maximum speed of a boat in still water is 27 km/h. Now this boat is moving downstream in a river flowing at 9 km/h. A man in the boat throws a ball vertically upwards with speed of 10 m/s. Range of the ball as observed by an observer at rest on the river bank is _________ cm. (Take \( g = 10 \, {m/s}^2 \)).
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: