Respuesta :
Answer:
Part a: [tex]f , \, f_y[/tex] is continuous at the initial value (0,0) so due to Picardi theorem there exists an interval such that the IVP has a unique solution.
Part b: [tex]f_y[/tex] is not continuous at the initial value (0,0) so due to Picardi theorem there does not exist an interval such that the IVP has a unique solution.
part c: [tex]f , \, f_y[/tex] is continuous at the initial value (0,1) so due to Picardi theorem there exists an interval such that the IVP has a unique solution.
Step-by-step explanation:
Part a
as [tex]y^{' }=ty^{4/3}[/tex]
Let
[tex]f(t,y)=ty^{4/3}[/tex]
Now derivative wrt y is given as
[tex]f_y=\frac{4}{3}ty^{1/3}[/tex]
Finding continuity via the initial value
[tex]f[/tex] is continuous on [tex]R^2[/tex] also [tex]f_y[/tex] is also continuous on [tex]R^2[/tex]
Also
[tex]f , \, f_y[/tex] is continuous at the initial value (0,0) so due to Picardi theorem there exists an interval such that the IVP has a unique solution.
Part b
as [tex]y^{' }=ty^{1/3}[/tex]
Let
[tex]f(t,y)=ty^{1/3}[/tex]
Now derivative wrt y is given as
[tex]f_y=\frac{1}{3}ty^{-2/3}[/tex]
Finding continuity via the initial value
[tex]f[/tex] is continuous on [tex]R^2[/tex] also [tex]f_y[/tex] is also continuous on [tex]R^2[/tex]
Also
[tex]f_y[/tex] is not continuous at the initial value (0,0) so due to Picardi theorem there does not exist an interval such that the IVP has a unique solution.
Part c
as [tex]y^{' }=ty^{1/3}[/tex]
Let
[tex]f(t,y)=ty^{1/3}[/tex]
Now derivative wrt y is given as
[tex]f_y=\frac{1}{3}ty^{-2/3}[/tex]
Finding continuity via the initial value
[tex]f[/tex] is continuous on [tex]R^2[/tex] also [tex]f_y[/tex] is also continuous on [tex]R^2[/tex] when [tex]y\neq 0[/tex]
Also
[tex]f , \, f_y[/tex] is continuous at the initial value (0,1) so due to Picardi theorem there exists an interval such that the IVP has a unique solution.