e+1/2 \(e+\frac {1}{2}\)
\(-\frac {1}{2}\)
We begin by determining the integrating factor (IF):
ex: IF=e−∫t1+tdt=e−∫t+11+tdt=e−t+log(1+t)=1+te−t.
The sought-after solution can be expressed as y(IF)=∫Q⋅IFdt+C, where Q=11+t is derived from the given equation.
Thus, y(IF)=∫11+t⋅1+te−tdt+C,
=∫e−tdt+C,
=−e−t+C.
Given the initial condition y(0)=−1, we find:
−1⋅(1+0)=−e0+C,
−1=−1+C,
C=0.
Plugging the value of C back in, we have:
y(IF)=−e−t+0,
=−e−t.
Evaluating at t=1:
y(IF)=−e−1,
\(=-\frac {1}{e}\)
above is example. but here proves that : \(-\frac {1}{2}\)
Two identical concave mirrors each of focal length $ f $ are facing each other as shown. A glass slab of thickness $ t $ and refractive index $ n_0 $ is placed equidistant from both mirrors on the principal axis. A monochromatic point source $ S $ is placed at the center of the slab. For the image to be formed on $ S $ itself, which of the following distances between the two mirrors is/are correct:
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