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The final particular solution is $X_p(t) = 2te^{-t}$. This is obtained by substituting the solved coefficient $A=2$ back into the resonant trial solution $x=Ate^{-t}$.

Conditions: The ODE is $\ddot{x}+3\dot{x}+2x=2e^{-t}$.; The coefficient $A$ has been determined to be $2$.; The trial solution form is $x=Ate^{-t}$.

The final particular solution is $X_p(t) = 2te^{-t}$. This is obtained by substituting the solved coefficient $A=2$ back into the resonant trial solution $x=Ate^{-t}$.

Conditions: The ODE is $\ddot{x}+3\dot{x}+2x=2e^{-t}$.; The coefficient $A$ has been determined to be $2$.; The trial solution form is $x=Ate^{-t}$.

Substitute the trial solution $x=Ate^{-t}$ and its derivatives into the ODE, factor out the common term $e^{-t}$, and collect like terms by powers of $t$. Equating the remaining constant term to the right-hand side yields $A=2$.

Conditions: The trial solution is $x=Ate^{-t}$.; The ODE is $\ddot{x}+3\dot{x}+2x=2e^{-t}$.; $e^{-t}$ is never zero, allowing it to be canceled from both sides.

Substitute the trial solution $x=Ate^{-t}$ and its derivatives into the ODE, factor out the common term $e^{-t}$, and collect like terms by powers of $t$. Equating the remaining constant term to the right-hand side yields $A=2$.

Conditions: The trial solution is $x=Ate^{-t}$.; The ODE is $\ddot{x}+3\dot{x}+2x=2e^{-t}$.; $e^{-t}$ is never zero, allowing it to be canceled from both sides.