(A)Rewrite the given differential equation: \[ \frac{dy}{dx} + \frac{1}{x \log_e x} y = x. \] (B)This is a linear differential equation of the form: \[ \frac{dy}{dx} + P(x)y = Q(x), \] where \( P(x) = \frac{1}{x \log_e x} \) and \( Q(x) = x \). (C)The integrating factor (I.F.) is given by: \[ \text{I.F.} = e^{\int P(x) dx} = e^{\int \frac{1}{x \log_e x} dx}. \] Substituting \( u = \log_e x \), \( du = \frac{1}{x} dx \), we get: \[ \int \frac{1}{x \log_e x} dx = \int \frac{1}{u} du = \log_e u = \log_e(\log_e x). \] Therefore: \[ \text{I.F.} = e^{\log_e(\log_e x)} = \log_e x. \] (D)Multiply through the differential equation by \( \log_e x \): \[ (\log_e x) \frac{dy}{dx} + \frac{y}{x} = x \log_e x. \] (E)Recognize the left-hand side as a derivative: \[ \frac{d}{dx}(y \log_e x) = x \log_e x. \] (F) Integrate both sides: \[ y \log_e x = \int x \log_e x \, dx. \] (G) Use integration by parts for \( \int x \log_e x \, dx \), letting \( u = \log_e x \) and \( dv = x dx \): \[ u = \log_e x, \, du = \frac{1}{x} dx, \, v = \frac{x^2}{2}. \] Then: \[ \int x \log_e x \, dx = \frac{x^2}{2} \log_e x - \int \frac{x^2}{2} \cdot \frac{1}{x} dx = \frac{x^2}{2} \log_e x - \frac{x^2}{4}. \] Substituting back: \[ y \log_e x = \frac{x^2}{2} \log_e x - \frac{x^2}{4} + C. \] Divide through by \( \log_e x \): \[ y = \frac{x^2}{2} - \frac{x^2}{4 \log_e x} + \frac{C}{\log_e x}. \] Use the initial condition \( y(2) = 2 \) to find \( C \). When \( x = 2 \), \( \log_e 2 \neq 0 \): \[ 2 = \frac{4}{2} - \frac{4}{4 \log_e 2} + \frac{C}{\log_e 2}. \] Simplify: \[ 2 = 2 - \frac{1}{\log_e 2} + \frac{C}{\log_e 2}. \] Solving for \( C \): \[ C = 1. \] The solution becomes: \[ y = \frac{x^2}{2} - \frac{x^2}{4 \log_e x} + \frac{1}{\log_e x}. \] (K) Evaluate \( y(e) \): \[ y(e) = \frac{e^2}{2} - \frac{e^2}{4 \log_e e} + \frac{1}{\log_e e}. \] Since \( \log_e e = 1 \): \[ y(e) = \frac{e^2}{2} - \frac{e^2}{4} + 1 = \frac{2e^2}{4} - \frac{e^2}{4} + 1 = \frac{e^2}{4} + 1. \] Simplify: \[ y(e) = \frac{4 + e^2}{4}. \]
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 Ξ©, 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:
A differential equation is an equation that contains one or more functions with its derivatives. The derivatives of the function define the rate of change of a function at a point. It is mainly used in fields such as physics, engineering, biology and so on.
The first-order differential equation has a degree equal to 1. All the linear equations in the form of derivatives are in the first order. It has only the first derivative such as dy/dx, where x and y are the two variables and is represented as: dy/dx = f(x, y) = yβ
The equation which includes second-order derivative is the second-order differential equation. It is represented as; d/dx(dy/dx) = d2y/dx2 = fβ(x) = yβ.
Differential equations can be divided into several types namely