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Answers for “共振试探解 $Ate^{-t}$ 的一阶和二阶导数是什么?”

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Meet the concept

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The first derivative is x˙=Ae−t(1−t)\dot{x}=Ae^{-t}(1-t), and the second derivative is x¨=Ae−t(t−2)\ddot{x}=Ae^{-t}(t-2). These are computed by applying the product rule successively to the trial solution x=Ate−tx=Ate^{-t}.

Conditions: The trial solution is x=Ate−tx=Ate^{-t}.; Differentiation is with respect to tt.; The product rule is applied to tt and e−te^{-t}.

Understand why

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The particular solution uses Ate−tAte^{-t} because the forcing term e−te^{-t} is already a solution to the associated homogeneous equation. In the method of undetermined coefficients, if the forcing function overlaps with a homogeneous solution (resonance), the standard guess must be multiplied by tt to ensure linear independence.

Conditions: The ODE is linear with constant coefficients.; The forcing term contains e−te^{-t}.; r=−1r=-1 is a root of the homogeneous characteristic equation.

Find a method

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The homogeneous roots are obtained by solving the associated homogeneous equation x¨+3x˙+2x=0\ddot{x}+3\dot{x}+2x=0. By substituting the exponential trial solution x=ertx=e^{rt}, the differential equation converts into the characteristic polynomial r2+3r+2=0r^2+3r+2=0, which factors to (r+2)(r+1)=0(r+2)(r+1)=0, yielding the roots r=−2r=-2 and r=−1r=-1.

Conditions: The ODE has constant coefficients.; The trial solution is of the form x=ertx=e^{rt}.; The characteristic equation is a quadratic polynomial.

Know when to use it

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The first segment stops after computing the first and second derivatives of the resonant trial solution x=Ate−tx=Ate^{-t}. It does not yet substitute these derivatives back into the differential equation or solve for the unknown coefficient AA.

Conditions: The segment covers the setup of the homogeneous solution and the resonant trial solution.; The derivatives x˙\dot{x} and x¨\ddot{x} are computed but not substituted.