Answer:
Part a: The equation is a linear first order differential equation as superposition and homogeneity is satisfied.
Part b: The solution of the differential equation is [tex]y(t)=\frac{u(t)-e^{-kt} u(t)}{k}[/tex]
Step-by-step explanation:
Part a:
Let us suppose the differential equation is given as
[tex]\frac{d}{dy} y(t) +k y(t)=u(t)[/tex]
For a solution, it is given as
[tex]\frac{d}{dy} y_1(t) +k y_1(t)=u_1(t)[/tex]
For another solution it is given as
[tex]\frac{d}{dy} y_2(t) +k y_2(t)=u_2(t)[/tex]
Adding these two solution gives
[tex]\frac{d}{dy} y_1(t) +k y_1(t)=u_1(t) \\+ \\\frac{d}{dy} y_2(t) +k y_2(t)=u_2(t)\\\\\frac{d}{dy} (y_1(t)+y_2(t)) +k (y_1(t)+y_2(t))=(u_1(t)+u_2(t))[/tex]
Which is also the solution of the equation and thus as superposition (additivity) and homogeneity is satisfied, so the equation is a linear first order differential equation.
Part b
[tex]\frac{d}{dy} y(t) +k y(t)=u(t)[/tex]
So taking Laplace on both sides
[tex]s Y(s)+kY(s)=\frac{1}{s}[/tex]
Here
[tex]u(t)=\frac{1}{s}[/tex]
Rearranging the equation gives
[tex]Y(s)=\frac{1}{k(s+k)}\\Y(s)=\frac{1}{k}[\frac{1}{s}-\frac{1}{s+k}]\\[/tex]
Taking inverse Laplace gives
[tex]y(t)=\frac{u(t)-e^{-kt} u(t)}{k}[/tex]
This is the solution of the differential equation.