1)
Given the system let us express y as a function of t.
i) 3dtdx+2dtdy−x+y=t−1
ii)dtdx+dtdy−x=t+2
Multiplying equation by ×3 , we get -
And the adding i) and ii) , we get -
=dt−dy+2x+y=−2t−7
It gives values of x as -
x=21dtdy−21y−t−27
Now , differentiating with respect to t , we get -
=dtdx= 21dt2d2y−21dtdy−1 .
We get the equation as -
=21dt2d2y−21dtdy−1+dtdy−(21dtdy−21y−t−27)=t+2
Which is equivalent to -
=21dt2d2y+21y=2−1
And hence the equation becomes -
=dt2d2y+y=−1
Auxiliary equation becomes -
=m2+1=0
It's root's becomes as -
m=+i,−i ,
It's follows that solution is of form -
=y(t)=C1cost+C2sint+yp, where yp=a
It's follows that -
dt2d2yp=0 , hence a=−1. Therefore the solution is the following -
y(t)=C1cost+C2sint−1
2)
Ordinary point of equation is defined as -
A point a is called ordinary point of differential equation when function p1(x) and p0(x) are analytical at x=a ,
=a0(x)dx2d2y+a1(x)dxdy+a2(x)y=0
For , the above equation the ordinary point is called as -
A point x=x0 is called ordinary point of differential equation if a0(x)=0 at x=x0 . The point x=x0 is called that ordinary point .
=(2x3−3)dx2d2y−2xdxdy+y=0 y(0)=−1
y′(1)=5
Now , we know that taylor's series expansion is expressed as -
y(x)= y(0)+y′(0)(x−0)+2!1y′′(0)(x−0)2+....
=y′′(x)=2x3−32xy′(x)−2x3−3y
Now putting , x=0, we get -
y′′(0)=0−−3y(0)
y′′(0)=3−1
y(x)=−1+5x+2!13−1x2+.........
This is taylor's series of given equation .
Comments