\(((tan−1y)−x)dy=(1+y^2)dx\)
\(\frac{dx}{dy}+\frac{x}{1+y^2}=\frac{tan^{−1}y}{1+y^2}\)
\(I.F.=e^{∫\frac{1}{1+y^2}dy}=e^{tan^{−1}y}\)
∴ Solution
\(x.e^{tan^{-1}y}∫\frac{e^{tan^{-1}}y^{tan^{-1}}y}{1+y^2}dy\)
Let
\(e^{tan^{−1}}y=t\)
\(\frac{e^{tan^{−1}y}}{1+y^2}=dt\)
=\(xe^{tan^{−1}y}∫ ln\; tdt =t \;ln t–t+c\)
=\(xe^{tan^{−1}y}=e^{tan^{−1}y}tan^{−1}y−e^{tan^{-1}y}+c…(i)\)
∵ It passes through \((1, 0) ⇒ c = 2\)
Now put \(y = tan1\), then
\(ex = e – e + 2\)
\(⇒x=\frac{2}{e}\)
Let $ y(x) $ be the solution of the differential equation $$ x^2 \frac{dy}{dx} + xy = x^2 + y^2, \quad x > \frac{1}{e}, $$ satisfying $ y(1) = 0 $. Then the value of $ 2 \cdot \frac{(y(e))^2}{y(e^2)} $ is ________.
A bob of mass \(m\) is suspended at a point \(O\) by a light string of length \(l\) and left to perform vertical motion (circular) as shown in the figure. Initially, by applying horizontal velocity \(v_0\) at the point ‘A’, the string becomes slack when the bob reaches at the point ‘D’. The ratio of the kinetic energy of the bob at the points B and C is:
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) = y’
The equation which includes second-order derivative is the second-order differential equation. It is represented as; d/dx(dy/dx) = d2y/dx2 = f”(x) = y”.
Differential equations can be divided into several types namely