Skip to content
Back to exploration
Mathematical modeling / English

Particular solution of an ode: resonance

Jeffrey Chasnov · YouTube · 5:34

Open original
READ & KEEP

The explanation, unpacked.

Saves 0

Reviewed learning material · Video analysis · English
Read the full overview

This whiteboard segment works on the nonhomogeneous ODE x¨+3x˙+2x=2e−t\ddot{x}+3\dot{x}+2x=2e^{-t} and focuses on the resonance issue in the method of undetermined coefficients. The presenter first solves the homogeneous equation via x=ertx=e^{rt}, obtaining (r+2)(r+1)=0(r+2)(r+1)=0 and hence xh(t)=c1e−2t+c2e−tx_h(t)=c_1e^{-2t}+c_2e^{-t}. Because the forcing term contains e−te^{-t}, the video explicitly shows that the naive particular guess must be multiplied by tt, leading to the trial xp(t)=Ate−tx_p(t)=Ate^{-t}. The remainder of the clip computes x˙p=Ae−t(1−t)\dot{x}_p=Ae^{-t}(1-t) and x¨p=Ae−t(−1+t−1)=Ae−t(t−2)\ddot{x}_p=Ae^{-t}(-1+t-1)=Ae^{-t}(t-2), stopping before substitution into the ODE and before determining the constant AA. This segment demonstrates finding a particular solution to the non-homogeneous ODE x¨+3x˙+2x=2e−t\ddot{x} + 3\dot{x} + 2x = 2e^{-t} using the method of undetermined coefficients. Because the forcing term e−te^{-t} resonates with the homogeneous solution, the trial form x = Ate^{-t} is used. The video substitutes this trial solution and its derivatives into the ODE, cancels the common factor e−te^{-t}, collects like terms, and solves for the coefficient A=2A = 2, yielding the final particular solution Xp(t)=2X_p(t) = 2te^{-t}. This 4-second clip shows a static whiteboard displaying the final algebraic steps for finding a particular solution to a second-order linear non-homogeneous ordinary differential equation using the method of undetermined coefficients. The equation x¨+3x˙+2x=2\ddot{x} + 3\dot{x} + 2x = 2 is solved by substituting an assumed form, leading to the coefficient A=2A = 2 and the final particular solution xp(t)=2x_p(t) = 2te^{-t}.

Use the learning inspector for key ideas and moments, or open the reading tabs for the complete notes.

Chapters

0:00Problem statement: find a particular solution0:23Homogeneous equation and characteristic roots0:50Homogeneous solution and resonance with e−te^{-t}1:15Modified trial xp=Ate−tx_p=Ate^{-t}1:45First derivative by the product rule2:10Second derivative and pending substitution2:45Resonant Trial Solution2:57Substitution and Simplification5:12Final Particular Solution5:30Solving for the Particular Solution

Learning script

Generated from the video's visuals and explanation; not verbatim speech.

The clip opens on the equation x¨+3x˙+2x=2e−t\ddot{x}+3\dot{x}+2x=2e^{-t} and states the immediate goal: find a particular solution, not the full general solution.

Before guessing that particular solution, the presenter checks the associated homogeneous equation, because the forcing term e−te^{-t} may already belong to the homogeneous solution space.

Using the standard exponential trial x=ertx=e^{rt}, the homogeneous equation leads to the characteristic polynomial r2+3r+2=0r^2+3r+2=0, which factors as (r+2)(r+1)=0(r+2)(r+1)=0.

Therefore the complementary solution is xh(t)=c1e−2t+c2e−tx_h(t)=c_1e^{-2t}+c_2e^{-t}. The board then visually links the forcing term 2e−t2e^{-t} to the homogeneous mode e−te^{-t}, showing the resonance problem.

Because of that overlap, the usual non-resonant guess Ae−tAe^{-t} is replaced by the modified ansatz xp(t)=Ate−tx_p(t)=Ate^{-t}, where AA is still unknown.

To prepare for substitution into the ODE, the first derivative is computed by the product rule: x˙p=Ae−t(1−t)\dot{x}_p=Ae^{-t}(1-t).

Differentiating once more gives x¨p=Ae−t(−1+t−1)\ddot{x}_p=Ae^{-t}(-1+t-1), which simplifies to Ae−t(t−2)Ae^{-t}(t-2). The segment stops here, before substituting these expressions back into the differential equation and solving for AA.

We begin with the trial particular solution x=Ate−tx = Ate^{-t}, chosen because the forcing term e−te^{-t} causes resonance with the homogeneous solution. Its derivatives are x˙=Ae−t(1−t)\dot{x} = Ae^{-t}(1-t) and x¨=Ae−t(−2+t)\ddot{x} = Ae^{-t}(-2+t).

Next, we substitute these expressions into the left-hand side of the differential equation x¨+3x˙+2x\ddot{x} + 3\dot{x} + 2x. This gives Ae−t(−2+t)+3Ae−t(1−t)+2Ate−t=2e−tAe^{-t}(-2+t) + 3Ae^{-t}(1-t) + 2Ate^{-t} = 2e^{-t}.

Since e−te^{-t} is never zero, we can divide both sides by e−te^{-t} to simplify the equation to A(−2+t)+3A(1−t)+2At=2A(-2+t) + 3A(1-t) + 2At = 2.

Now we collect like terms. The terms proportional to tt are At−3At+2AtAt - 3At + 2At, which sum to 0t0t and cancel out completely. The constant terms are −2A+3A-2A + 3A, which simplify to AA.

Equating the remaining constant term to the right-hand side gives A=2A = 2. Substituting this back into our initial guess, we find the particular solution is Xp(t)=2te−tX_p(t) = 2te^{-t}.

The whiteboard displays the differential equation x¨+3x˙+2x=2\ddot{x} + 3\dot{x} + 2x = 2. Below it, the substitution step is shown as (A−3A+2A)t+(−2A+3A)=2(A - 3A + 2A)t + (-2A + 3A) = 2, which simplifies to yield A=2A = 2. The final particular solution is written at the bottom as xp(t)=2te−tx_p(t) = 2te^{-t}.

Knowledge cards

01

Resonance in a second-order linear ODE

For x¨+3x˙+2x=2e−t\ddot{x}+3\dot{x}+2x=2e^{-t}, the forcing exponential e−te^{-t} is not independent of the homogeneous solution. The video first solves the homogeneous equation and finds xh(t)=c1e−2t+c2e−tx_h(t)=c_1e^{-2t}+c_2e^{-t}, so e−te^{-t} is already present. That overlap is the reason the particular-solution trial must be modified.

x¨+3x˙+2x=2e−t\ddot{x}+3\dot{x}+2x=2e^{-t}
02

Characteristic equation from the exponential trial

Trying x=ertx=e^{rt} in the homogeneous equation produces r2+3r+2=0r^2+3r+2=0, which factors as (r+2)(r+1)=0(r+2)(r+1)=0. Hence the roots are r=−2r=-2 and r=−1r=-1, giving the two homogeneous modes e−2te^{-2t} and e−te^{-t}.

x=ert⇒r2+3r+2=0⇒(r+2)(r+1)=0x=e^{rt}\Rightarrow r^2+3r+2=0\Rightarrow (r+2)(r+1)=0
03

Why the particular guess becomes Ate−tAte^{-t}

In the method of undetermined coefficients, if the forcing term duplicates a homogeneous solution, the naive guess must be multiplied by tt. Here the duplicate mode is e−te^{-t}, so the correct trial is xp(t)=Ate−tx_p(t)=Ate^{-t} rather than Ae−tAe^{-t}.

xp(t)=Ate−tx_p(t)=Ate^{-t}
04

Derivatives needed before substitution

The clip computes the derivatives of the resonant trial solution. First, x˙p=Ae−t(1−t)\dot{x}_p=Ae^{-t}(1-t). Second, x¨p=Ae−t(−1+t−1)=Ae−t(t−2)\ddot{x}_p=Ae^{-t}(-1+t-1)=Ae^{-t}(t-2). These are the expressions that would next be substituted into the ODE to determine AA, but that final step is not shown in this segment.

x˙p=Ae−t(1−t),x¨p=Ae−t(t−2)\dot{x}_p=Ae^{-t}(1-t),\quad \ddot{x}_p=Ae^{-t}(t-2)
05

Resonant Trial Solution

When solving a non-homogeneous linear ODE with constant coefficients, if the forcing function shares a form with the homogeneous solution (resonance), the standard trial guess must be multiplied by tt. Here, since e−te^{-t} is in the homogeneous solution, the trial particular solution is x=Ate−tx = Ate^{-t} rather than x=Ae−tx = Ae^{-t}.

x=Ate−tx = Ate^{-t}
06

Substituting into the ODE

To find the undetermined coefficient AA, substitute the trial solution and its derivatives into the original differential equation. For x¨+3x˙+2x=2e−t\ddot{x} + 3\dot{x} + 2x = 2e^{-t}, using x=Ate−tx = Ate^{-t}, x˙=Ae−t(1−t)\dot{x} = Ae^{-t}(1-t), and x¨=Ae−t(−2+t)\ddot{x} = Ae^{-t}(-2+t) leads to an equation where e−te^{-t} can be canceled from all terms.

Ae−t(−2+t)+3Ae−t(1−t)+2Ate−t=2e−tAe^{-t}(-2+t) + 3Ae^{-t}(1-t) + 2Ate^{-t} = 2e^{-t}
07

Collecting Terms and Solving for A

After canceling e−te^{-t}, expand and group the remaining expression by powers of tt. The coefficients of tt will sum to zero due to the properties of the characteristic equation in resonant cases. The remaining constant terms are set equal to the right-hand side constant to solve for AA. In this example, −2A+3A=2-2A + 3A = 2 yields A=2A = 2.

(A−3A+2A)t+(−2A+3A)=2  ⟹  A=2(A - 3A + 2A)t + (-2A + 3A) = 2 \implies A = 2
08

Final Particular Solution

Once the coefficient AA is determined, substitute it back into the trial form to state the final particular solution. With A=2A=2, the particular solution for the given ODE is Xp(t)=2te−tX_p(t) = 2te^{-t}.

Xp(t)=2te−tX_p(t) = 2te^{-t}
09

Particular Solution via Undetermined Coefficients

To solve the non-homogeneous ODE x¨+3x˙+2x=2\ddot{x} + 3\dot{x} + 2x = 2, we assume a particular solution form and substitute it into the equation. Grouping the terms by powers of tt gives (A−3A+2A)t+(−2A+3A)=2(A - 3A + 2A)t + (-2A + 3A) = 2. The coefficient of tt becomes 00, and the constant term becomes AA. Setting A=2A = 2 allows us to write the final particular solution as xp(t)=2te−tx_p(t) = 2te^{-t}.

xp(t)=2te−tx_p(t) = 2te^{-t}

Detailed learning notes

Explore conditions, steps and evidence. Supplementary explanations are labeled separately from content shown in the video.

Symbols · 18

x

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    The dependent variable is written as x in the displayed ODE and in the trial solutions.

Symbol

x

Meaning

Unknown function of t in the differential equation.

Domain

Function of t; domain not explicitly stated in the clip.

t

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    The independent variable appears as t in e−te^{-t}, e^{rt}, and the trial particular solution Ate−tA t e^{-t}.

Symbol

t

Meaning

Independent variable (time-like parameter) of the ODE.

Domain

Real variable; no explicit interval is shown.

x˙\dot{x}

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    The first derivative is written as x˙\dot{x} in the ODE and later computed explicitly.

Symbol

x˙\dot{x}

Meaning

First derivative of x with respect to t.

Domain

Defined wherever x is differentiable.

x¨\ddot{x}

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    The second derivative is written as x¨\ddot{x} in the ODE and later computed explicitly.

Symbol

x¨\ddot{x}

Meaning

Second derivative of x with respect to t.

Domain

Defined wherever x is twice differentiable.

r

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    r appears in the trial homogeneous solution x=ex=e^{rt} and in the characteristic polynomial r2+3r+2=0r^2+3r+2=0.

Symbol

r

Meaning

Exponential rate parameter used in the homogeneous trial solution.

Domain

Algebraic unknown solved from the characteristic equation.

c1c_1

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    c1c_1 multiplies e−2te^{-2t} in the displayed homogeneous solution.

Symbol

c1c_1

Meaning

Arbitrary constant multiplying the homogeneous mode e−2te^{-2t}.

Domain

Constant of integration; numerical value not specified.

c2c_2

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    c2c_2 multiplies e−te^{-t} in the displayed homogeneous solution.

Symbol

c2c_2

Meaning

Arbitrary constant multiplying the homogeneous mode e−te^{-t}.

Domain

Constant of integration; numerical value not specified.

A

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    A is introduced as the unknown coefficient in the trial particular solution x=Ate−tx=A t e^{-t}.

Uncertainties
  1. The final value of A is not reached within this clip.

Symbol

A

Meaning

Undetermined coefficient for the resonant particular-solution ansatz.

Domain

Constant to be determined by substitution into the ODE.

x

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    The variable x appears as the dependent function in the differential equation and trial solution.

Symbol

x

Meaning

Dependent variable (function of t) in the ordinary differential equation.

Domain

Real-valued function of t.

t

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    The variable t appears as the independent variable in e−te^{-t} and te^{-t}.

Symbol

t

Meaning

Independent variable (time).

Domain

Real numbers.

A

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    The constant A is introduced in the trial particular solution x = Ate^{-t} and solved for later.

Symbol

A

Meaning

Undetermined coefficient to be solved for in the particular solution.

Domain

Real constant.

x˙\dot{x}

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    The notation x˙\dot{x} appears in the differential equation and its derivative expression.

Symbol

x˙\dot{x}

Meaning

First derivative of x with respect to t.

Domain

Real-valued function of t.

Knowledge points · 11

Nonhomogeneous second-order linear ODE with exponential forcing

Clear evidence
Shown in the video
Evidence
  1. Audio
    Observation

    The speaker says they want to find a particular solution of x double dot plus 3 x dot plus 2 x equals 2 times e to the minus t.

  2. Formula
    Observation

    The board shows x¨+3x˙+2x=2e−t\ddot{x}+3\dot{x}+2x=2e^{-t}.

Definition
Explanation

The clip studies the differential equation x¨+3x˙+2x=2e−t\ddot{x}+3\dot{x}+2x=2e^{-t} and specifically seeks a particular solution rather than the full general solution. The forcing term is exponential, and the speaker immediately flags that its exponent matches one of the homogeneous modes.

Formula
x¨+3x˙+2x=2e−t\ddot{x}+3\dot{x}+2x=2e^{-t}
Conditions
  1. Linear second-order ODE with constant coefficients.

  2. Right-hand side is 2e−t2e^{-t}.

  3. Goal in this clip is only to set up and begin computing a particular solution.

Characteristic-equation method for the homogeneous ODE

Clear evidence
Shown in the video
Evidence
  1. Audio
    Observation

    The speaker says, 'for the homogeneous equation if we just try x equals e to the rt, we get the characteristic equation r squared plus 3r plus 2 equals 0'.

  2. Formula
    Observation

    The board writes 'hom eq: Try x=ex = e^{rt}' and then 'r2+3r+2=0r^2 + 3r + 2 = 0 => (r+2r+2)(r+1r+1)=0'.

Method
Explanation

To solve the associated homogeneous equation, the video uses the standard exponential trial x=ertx=e^{rt}. Substitution produces the characteristic polynomial r2+3r+2=0r^2+3r+2=0, which factors as (r+2)(r+1)=0(r+2)(r+1)=0. This identifies the two homogeneous exponents r=−2r=-2 and r=−1r=-1.

Formula
x=ert⇒r2+3r+2=0⇒(r+2)(r+1)=0x=e^{rt}\quad\Rightarrow\quad r^2+3r+2=0\quad\Rightarrow\quad (r+2)(r+1)=0
Conditions
  1. Applies to the homogeneous equation associated with constant-coefficient linear ODEs.

  2. Distinct real roots are obtained here.

Prerequisites
  1. Nonhomogeneous second-order linear ODE with exponential forcing

Homogeneous solution and overlap with the forcing term

Clear evidence
Shown in the video
Evidence
  1. Audio
    Observation

    The speaker states the homogeneous solution is some constant times e−2te^{-2t} plus another constant times e−te^{-t}.

  2. Formula
    Observation

    The board displays xh(t)=c1e−2t+c2e−tx_h(t)=c_1 e^{-2t}+c_2 e^{-t}.

  3. Diagram
    Observation

    An arrow is drawn from the forcing term 2e−t2e^{-t} toward the e−te^{-t} term in the homogeneous solution.

Formula
Explanation

From the roots r=−2r=-2 and r=−1r=-1, the homogeneous solution is written as xh(t)=c1e−2t+c2e−tx_h(t)=c_1e^{-2t}+c_2e^{-t}. The visual arrow emphasizes that the forcing term 2e−t2e^{-t} shares the same exponential factor as one homogeneous mode, so the usual non-resonant guess would fail.

Formula
xh(t)=c1e−2t+c2e−tx_h(t)=c_1e^{-2t}+c_2e^{-t}
Conditions
  1. Roots of the characteristic equation are distinct and real.

  2. This is the complementary solution of the homogeneous ODE.

Prerequisites
  1. Characteristic-equation method for the homogeneous ODE

Resonance-adjusted trial for the particular solution

Clear evidence
Shown in the video
Evidence
  1. Audio
    Observation

    The speaker says that to find the particular solution, they must try x equal to some unknown coefficient and multiply the right-hand side by t, giving Ate−tA t e^{-t}.

  2. Formula
    Observation

    The board writes 'Part sol: Try x=Ate−tx = A t e^{-t}'.

Method
Explanation

Because e−te^{-t} already solves the homogeneous equation, the video modifies the usual undetermined-coefficients guess by multiplying by tt. The chosen ansatz is xp(t)=Ate−tx_p(t)=Ate^{-t}, where AA is the unknown coefficient to be determined after substitution into the ODE.

Formula
xp(t)=Ate−tx_p(t)=Ate^{-t}
Conditions
  1. Use when the forcing term overlaps a homogeneous solution mode.

  2. Here the overlap is with e−te^{-t}, so one factor of tt is inserted.

Prerequisites
  1. Homogeneous solution and overlap with the forcing term

First derivative of the resonant trial solution

Clear evidence
Shown in the video
Evidence
  1. Audio
    Observation

    The speaker verbally applies the product rule: derivative of the first times the second plus the first times derivative of the second.

  2. Formula
    Observation

    The board shows x˙\dot{x}=Ae^{-t}(1-t).

Formula
Explanation

Differentiating x=Ate−tx=Ate^{-t} with the product rule gives x˙=Ae−t−Ate−t=Ae−t(1−t)\dot{x}=Ae^{-t}-Ate^{-t}=Ae^{-t}(1-t). This expression is then used to compute the second derivative.

Formula
x˙=Ae−t(1−t)\dot{x}=Ae^{-t}(1-t)
Conditions
  1. Differentiate with respect to t.

  2. Product rule applied to tt and e−te^{-t}.

Prerequisites
  1. Resonance-adjusted trial for the particular solution

Second derivative of the resonant trial solution

Clear evidence
Shown in the video
Evidence
  1. Audio
    Observation

    The speaker again uses the product rule and says the result is minus one plus t plus the first times derivative of the second, giving minus one.

  2. Formula
    Observation

    The board shows x¨\ddot{x}=Ae^{-t}(-1+t-1).

  3. Diagram
    Observation

    A brace groups the terms inside the parentheses as the speaker comments on the combination.

Uncertainties
  1. The unsimplified form is shown, but the clip ends before the simplified second derivative or substituted ODE result is written.

Formula
Explanation

Differentiating x˙=Ae−t(1−t)\dot{x}=Ae^{-t}(1-t) once more yields x¨=Ae−t(−1+t−1)\ddot{x}=Ae^{-t}(-1+t-1). The bracketed terms combine to t−2t-2, so the simplified form is x¨=Ae−t(t−2)\ddot{x}=Ae^{-t}(t-2), although the simplification is not fully completed on screen within this clip.

Formula
x¨=Ae−t(−1+t−1)=Ae−t(t−2)\ddot{x}=Ae^{-t}(-1+t-1)=Ae^{-t}(t-2)
Conditions
  1. Continue from the previously computed first derivative.

  2. Product rule applied again to e−te^{-t} and (1−t)(1-t).

Prerequisites
  1. First derivative of the resonant trial solution

Trial Particular Solution Form

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    The board shows 'Part sol. Try x = Ate^{-t}' along with its first and second derivatives.

Method
Explanation

For a non-homogeneous term proportional to e−te^{-t}, when -1 is a root of the characteristic equation, the standard method of undetermined coefficients multiplies the usual guess by t. The video uses this resonant form x = Ate^{-t}.

Formula
x=Ate−tx = Ate^{-t}
Conditions
  1. The forcing term contains e−te^{-t}.

  2. -1 is a simple root of the homogeneous characteristic equation.

Substituting Trial Solution into ODE

Clear evidence
Shown in the video
Evidence
  1. Audio
    Observation

    The speaker says, 'So we substitute into the differential equation, so x double dot plus 3x dot plus 2x.'

  2. Formula
    Observation

    The left-hand side operator x¨+3x˙+2x\ddot{x} + 3\dot{x} + 2x is rewritten below the trial solution block.

Method
Explanation

The candidate particular solution and its derivatives are substituted into the left-hand side of the original differential equation to determine the unknown coefficient A.

Formula
x¨+3x˙+2x\ddot{x} + 3\dot{x} + 2x
Conditions
  1. x, x˙\dot{x}, and x¨\ddot{x} are evaluated using the trial form x = Ate^{-t}.

Prerequisites
  1. Trial Particular Solution Form

Collecting Like Terms After Substitution

Clear evidence
Shown in the video
Evidence
  1. Audio
    Observation

    The speaker explains collecting terms proportional to t and terms not proportional to t after canceling e−te^{-t}.

  2. Formula
    Observation

    The board shows the grouped expression (A−3A+2AA - 3A + 2A)t+(−2A+3A)t + (-2A + 3A).

Method
Explanation

After substituting the trial solution and factoring out e−te^{-t}, the resulting expression is organized into coefficients of t and constant terms. This allows matching against the right-hand side of the differential equation.

Formula
(A−3A+2A)t+(−2A+3A)(A - 3A + 2A)t + (-2A + 3A)
Conditions
  1. The common factor e−te^{-t} has been canceled from both sides.

Prerequisites
  1. Substituting Trial Solution into ODE

Second-order linear non-homogeneous ODE

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    x¨+3x˙+2x=2\ddot{x} + 3\dot{x} + 2x = 2

Definition
Explanation

The video displays a second-order linear ordinary differential equation with constant coefficients and a constant non-homogeneous term on the right side.

Formula
x¨+3x˙+2x=2\ddot{x} + 3\dot{x} + 2x = 2
Conditions
  1. The equation is linear.

  2. The coefficients are constants (1, 3, 2).

  3. The right-hand side is a constant (2).

Method of Undetermined Coefficients

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    Substitution of terms involving A into the ODE to solve for A.

Uncertainties
  1. The exact assumed form of the particular solution before substitution is not explicitly written out in the visible frame.

Method
Explanation

A technique for finding a particular solution to a non-homogeneous linear ODE by assuming a solution form with unknown coefficients, substituting it into the ODE, and solving for those coefficients.

Formula
Conditions
  1. Applies to linear ODEs with constant coefficients.

  2. The non-homogeneous term must be of a specific type (e.g., polynomial, exponential, sine/cosine).

Prerequisites
  1. Second-order linear non-homogeneous ODE
Claims and conditions · 2

The forcing exponential is already a homogeneous mode

Clear evidence
Shown in the video
Evidence
  1. Audio
    Observation

    The speaker says the complication is that e−te^{-t} is a solution of the homogeneous equation.

  2. Formula
    Observation

    The homogeneous solution contains the term c2e−tc_2 e^{-t}.

  3. Diagram
    Observation

    An arrow visually links the forcing term 2e−t2e^{-t} to the e−te^{-t} part of xh(t)x_h(t).

Proposition
Statement

For the ODE x¨+3x˙+2x=2e−t\ddot{x}+3\dot{x}+2x=2e^{-t}, the forcing factor e−te^{-t} belongs to the homogeneous solution space because r=−1r=-1 is a root of the characteristic equation.

Hypotheses
  1. Consider the associated homogeneous equation x¨+3x˙+2x=0\ddot{x}+3\dot{x}+2x=0.

  2. Use the exponential trial x=ertx=e^{rt}.

  3. The characteristic equation is r2+3r+2=0r^2+3r+2=0.

Quantifiers

For this specific ODE and its homogeneous solution.

Resonant forcing requires a t-multiplied particular-solution ansatz

Clear evidence
Shown in the video
Evidence
  1. Audio
    Observation

    The speaker says they need to multiply now the right hand side by t, giving Ate−tA t e^{-t}.

  2. Formula
    Observation

    The board writes Part sol: Try x=Ate−tx = A t e^{-t}.

Uncertainties
  1. The clip demonstrates the rule in this example but does not state a general theorem with full hypotheses.

Proposition
Statement

When the forcing term has the same exponential factor as a homogeneous solution, the trial particular solution is modified by multiplying by tt; here the chosen form is xp(t)=Ate−tx_p(t)=Ate^{-t}.

Hypotheses
  1. The ODE is linear with constant coefficients.

  2. The nonhomogeneous term contains a factor already present in the homogeneous solution.

Quantifiers

Stated for the worked example in the clip; the broader general rule is implied but not formally proved here.

Derivations and proofs · 4

Derivation of the characteristic equation and its roots

Clear evidence
Shown in the video
Evidence
  1. Audio
    Observation

    The speaker says trying x=ex=e^{rt} gives the characteristic equation r2+3r+2=0r^2+3r+2=0, which factors to (r+2r+2)(r+1r+1)=0.

  2. Formula
    Observation

    The board shows hom eq: Try x=ex=e^{rt}, then r2+3r+2=0r^2+3r+2=0 => (r+2r+2)(r+1r+1)=0.

Proof
Steps
  1. Expression
    x¨+3x˙+2x=0\ddot{x}+3\dot{x}+2x=0
    Explanation

    Start from the homogeneous version of the given ODE.

    Justification

    Associated homogeneous equation of the displayed nonhomogeneous ODE.

    Shown in the video
  2. Expression
    x=ertx=e^{rt}
    Explanation

    Try an exponential solution.

    Justification

    Standard method for constant-coefficient linear ODEs, as stated in the video.

    Shown in the video
  3. Expression
    r2+3r+2=0r^2+3r+2=0
    Explanation

    Substitution yields the characteristic polynomial.

    Justification

    Audio explicitly says this is the characteristic equation obtained from the trial.

    Shown in the video
  4. Expression
    (r+2)(r+1)=0(r+2)(r+1)=0
    Explanation

    Factor the quadratic.

    Justification

    Algebraic factorization shown on the board.

    Shown in the video
  5. Expression
    r=−2, r=−1r=-2,\ r=-1
    Explanation

    Read off the two roots.

    Justification

    Zero-product property applied to the factored equation.

    Derived from the video
Conclusion

The homogeneous exponents are r=−2r=-2 and r=−1r=-1, leading to the complementary solution built from e−2te^{-2t} and e−te^{-t}.

Differentiation of the resonant trial solution

Clear evidence
Shown in the video
Evidence
  1. Audio
    Observation

    The speaker verbally computes the first and second derivatives using the product rule.

  2. Formula
    Observation

    The board writes x=Ate^{-t}, then x˙\dot{x}=Ae^{-t}(1-t), then x¨\ddot{x}=Ae^{-t}(-1+t-1).

Uncertainties
  1. The clip stops before substituting these derivatives back into the ODE and solving for A.

Proof
Steps
  1. Expression
    x=Ate−tx=Ate^{-t}
    Explanation

    Begin with the chosen particular-solution ansatz.

    Justification

    Selected because e−te^{-t} overlaps the homogeneous solution.

    Shown in the video
  2. Expression
    x˙=Ae−t−Ate−t\dot{x}=Ae^{-t}-Ate^{-t}
    Explanation

    Apply the product rule to tt and e−te^{-t}.

    Justification

    Speaker explicitly describes derivative of the first times the second plus the first times derivative of the second.

    Shown in the video
  3. Expression
    x˙=Ae−t(1−t)\dot{x}=Ae^{-t}(1-t)
    Explanation

    Factor out Ae−tAe^{-t}.

    Justification

    Algebraic simplification shown on the board.

    Shown in the video
  4. Expression
    x¨=Ae−t(−1)+(Ae−t)(−1)+A(−e−t)(1−t)\ddot{x}=Ae^{-t}(-1)+(Ae^{-t})(-1)+A(-e^{-t})(1-t)
    Explanation

    Differentiate x˙=Ae−t(1−t)\dot{x}=Ae^{-t}(1-t) again using the product rule.

    Justification

    This is the standard expansion corresponding to the spoken derivation; the board presents the collected result rather than every intermediate line.

    Derived from the video
  5. Expression
    x¨=Ae−t(−1+t−1)\ddot{x}=Ae^{-t}(-1+t-1)
    Explanation

    Collect terms into the displayed bracketed form.

    Justification

    Matches the formula written on the board.

    Shown in the video
  6. Expression
    x¨=Ae−t(t−2)\ddot{x}=Ae^{-t}(t-2)
    Explanation

    Simplify the bracket.

    Justification

    Arithmetic simplification of −1+t−1=t−2-1+t-1=t-2; this final simplification is not fully written before the clip ends.

    Derived from the video
Conclusion

The trial particular solution has derivatives x˙=Ae−t(1−t)\dot{x}=Ae^{-t}(1-t) and x¨=Ae−t(t−2)\ddot{x}=Ae^{-t}(t-2), setting up the next step of substitution into the ODE.

Derivation of Coefficient A

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    The board displays the step-by-step substitution and simplification leading to A=2A = 2.

  2. Audio
    Observation

    The speaker narrates the cancellation of the t-proportional terms and the solving of the remaining equation.

Proof
Steps
  1. Expression
    x¨+3x˙+2x=2e−t\ddot{x} + 3\dot{x} + 2x = 2e^{-t}
    Explanation

    Start with the original non-homogeneous differential equation.

    Justification

    Given problem statement visible on the board.

    Shown in the video
  2. Expression
    x=Ate−t,x˙=Ae−t(1−t),x¨=Ae−t(−2+t)x = Ate^{-t}, \quad \dot{x} = Ae^{-t}(1-t), \quad \ddot{x} = Ae^{-t}(-2+t)
    Explanation

    Use the trial particular solution and its computed first and second derivatives.

    Justification

    Method of undetermined coefficients for a resonant forcing term.

    Shown in the video
  3. Expression
    Ae−t(−2+t)+3Ae−t(1−t)+2Ate−t=2e−tAe^{-t}(-2+t) + 3Ae^{-t}(1-t) + 2Ate^{-t} = 2e^{-t}
    Explanation

    Substitute x, x˙\dot{x}, and x¨\ddot{x} into the left-hand side of the ODE.

    Justification

    Direct algebraic substitution.

    Shown in the video
  4. Expression
    e−t[A(−2+t)+3A(1−t)+2At]=2e−te^{-t} [ A(-2+t) + 3A(1-t) + 2At ] = 2e^{-t}
    Explanation

    Factor out the common exponential term e−te^{-t}.

    Justification

    Distributive property of multiplication over addition.

    Derived from the video
  5. Expression
    A(−2+t)+3A(1−t)+2At=2A(-2+t) + 3A(1-t) + 2At = 2
    Explanation

    Divide both sides by e−te^{-t} (which is never zero) to simplify the equation.

    Justification

    Algebraic cancellation of a non-zero common factor.

    Shown in the video
  6. Expression
    (A−3A+2A)t+(−2A+3A)=2(A - 3A + 2A)t + (-2A + 3A) = 2
    Explanation

    Expand and collect terms by powers of t.

    Justification

    Polynomial grouping.

    Shown in the video
  7. Expression
    0⋅t+A=20 \cdot t + A = 2
    Explanation

    Simplify the coefficients: A−3A+2A=0A - 3A + 2A = 0 and -2A + 3A=A3A = A.

    Justification

    Arithmetic simplification.

    Shown in the video
  8. Expression
    A=2A = 2
    Explanation

    Solve the resulting linear equation for the undetermined coefficient.

    Justification

    Basic algebra.

    Shown in the video
Conclusion

The undetermined coefficient in the trial particular solution is A=2A = 2.

Solving for the undetermined coefficient A

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    = (A−3A+2AA - 3A + 2A)t+(−2A+3A)=2⇒A=2t + (-2A + 3A) = 2 \Rightarrow A = 2

Uncertainties
  1. The initial guess for the particular solution is not shown, but the algebraic steps imply a specific form was substituted.

Proof
Steps
  1. Expression
    (A−3A+2A)t+(−2A+3A)=2(A - 3A + 2A)t + (-2A + 3A) = 2
    Explanation

    After substituting the assumed particular solution and its derivatives into the ODE, the terms are grouped by powers of t.

    Justification

    Algebraic simplification and grouping like terms.

    Shown in the video
  2. Expression
    0⋅t+A=20 \cdot t + A = 2
    Explanation

    The coefficient of t simplifies to zero (A−3A+2A=0A - 3A + 2A = 0), and the constant term simplifies to A(−2A+3A=A)A (-2A + 3A = A).

    Justification

    Arithmetic calculation.

    Derived from the video
  3. Expression
    A=2A = 2
    Explanation

    Equating the remaining constant term to the right-hand side of the ODE yields the value of A.

    Justification

    Equality of polynomials/functions.

    Shown in the video
Conclusion

The undetermined coefficient A is equal to 2.

Worked examples · 2

Worked example: particular solution setup for x¨+3x˙+2x=2e−t\ddot{x}+3\dot{x}+2x=2e^{-t}

Clear evidence
Shown in the video
Evidence
  1. Audio
    Observation

    The entire clip is a worked example of finding a particular solution for the displayed ODE.

  2. Formula
    Observation

    The board carries the example from the ODE through the homogeneous solution, resonant ansatz, and derivative computations.

Uncertainties
  1. The example is unfinished within this clip because the coefficient A is not solved before the video segment ends.

Problem

Find a particular solution of x¨+3x˙+2x=2e−t\ddot{x}+3\dot{x}+2x=2e^{-t} when the forcing exponential overlaps a homogeneous solution.

Given
  1. The ODE is x¨+3x˙+2x=2e−t\ddot{x}+3\dot{x}+2x=2e^{-t}.

  2. The associated homogeneous equation has characteristic polynomial r2+3r+2=0r^2+3r+2=0.

  3. The homogeneous solution is xh(t)=c1e−2t+c2e−tx_h(t)=c_1e^{-2t}+c_2e^{-t}.

Goal

Set up the correct resonant trial for a particular solution and compute the derivatives needed for substitution.

Steps
  1. Expression
    r2+3r+2=0⇒(r+2)(r+1)=0r^2+3r+2=0\Rightarrow (r+2)(r+1)=0
    Explanation

    Solve the homogeneous characteristic equation.

    Justification

    Shown directly on the board after trying x=ertx=e^{rt}.

    Shown in the video
  2. Expression
    xh(t)=c1e−2t+c2e−tx_h(t)=c_1e^{-2t}+c_2e^{-t}
    Explanation

    Write the homogeneous solution from the two roots.

    Justification

    Standard consequence of distinct real roots; displayed on the board.

    Shown in the video
  3. Expression
    xp(t)=Ate−tx_p(t)=Ate^{-t}
    Explanation

    Because e−te^{-t} is already a homogeneous mode, multiply the naive guess by tt.

    Justification

    Explicitly stated by the speaker as the needed modification for resonance.

    Shown in the video
  4. Expression
    x˙p=Ae−t(1−t)\dot{x}_p=Ae^{-t}(1-t)
    Explanation

    Differentiate the trial solution once.

    Justification

    Product rule applied in the audio and written on the board.

    Shown in the video
  5. Expression
    x¨p=Ae−t(−1+t−1)\ddot{x}_p=Ae^{-t}(-1+t-1)
    Explanation

    Differentiate again.

    Justification

    Product rule applied a second time; the unsimplified form is shown on the board.

    Shown in the video
Answer

The clip establishes the correct resonant ansatz xp(t)=Ate−tx_p(t)=Ate^{-t} and computes x˙p=Ae−t(1−t)\dot{x}_p=Ae^{-t}(1-t) and x¨p=Ae−t(−1+t−1)=Ae−t(t−2)\ddot{x}_p=Ae^{-t}(-1+t-1)=Ae^{-t}(t-2), but it does not reach the final value of AA.

Verification

Verification would require substituting xpx_p, x˙p\dot{x}_p, and x¨p\ddot{x}_p into the original ODE and matching coefficients of e−te^{-t}; that step is not shown in this segment.

Finding the Particular Solution via Undetermined Coefficients

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    The entire segment is dedicated to solving for the particular solution of x¨+3x˙+2x=2e−t\ddot{x} + 3\dot{x} + 2x = 2e^{-t}.

Problem

Find a particular solution to the differential equation x¨+3x˙+2x=2e−t\ddot{x} + 3\dot{x} + 2x = 2e^{-t}.

Given
  1. The differential equation is x¨+3x˙+2x=2e−t\ddot{x} + 3\dot{x} + 2x = 2e^{-t}.

  2. The homogeneous solution contains the term e−te^{-t}, indicating resonance with the forcing function.

Goal

Determine the specific form and coefficient of the particular solution Xp(t)X_p(t).

Steps
  1. Expression
    x=Ate−tx = Ate^{-t}
    Explanation

    Propose a trial solution multiplied by t due to resonance.

    Justification

    Standard rule for undetermined coefficients when the forcing exponent matches a homogeneous root.

    Shown in the video
  2. Expression
    x˙=Ae−t(1−t),x¨=Ae−t(−2+t)\dot{x} = Ae^{-t}(1-t), \quad \ddot{x} = Ae^{-t}(-2+t)
    Explanation

    Compute the necessary derivatives of the trial solution.

    Justification

    Product rule and chain rule of differentiation.

    Shown in the video
  3. Expression
    (A−3A+2A)t+(−2A+3A)=2(A - 3A + 2A)t + (-2A + 3A) = 2
    Explanation

    Substitute into the ODE, cancel e−te^{-t}, and group like terms.

    Justification

    Algebraic manipulation and equating coefficients.

    Shown in the video
  4. Expression
    A=2A = 2
    Explanation

    Solve for the unknown coefficient A.

    Justification

    Simplifying the grouped equation yields A=2A = 2.

    Shown in the video
  5. Expression
    Xp(t)=2te−tX_p(t) = 2te^{-t}
    Explanation

    Write the final particular solution by substituting A back into the trial form.

    Justification

    Definition of the particular solution based on the solved coefficient.

    Shown in the video
Answer

Xp(t)=2X_p(t) = 2te^{-t}

Verification

Substituting Xp(t)=2X_p(t) = 2te^{-t} and its derivatives back into the original ODE satisfies the equation.

Visual events · 5

Visual link between forcing term and homogeneous mode

Clear evidence
Shown in the video
Evidence
  1. Diagram
    Observation

    An arrow is drawn from the forcing term 2e−t2e^{-t} in the top equation toward the e−te^{-t} term in the homogeneous solution.

Objects
  1. Top equation x¨+3x˙+2x=2e−t\ddot{x}+3\dot{x}+2x=2e^{-t}

  2. Homogeneous solution xh(t)=c1e−2t+c2e−tx_h(t)=c_1e^{-2t}+c_2e^{-t}

  3. Arrow annotation

Changes
  1. A new arrow annotation appears connecting the right-hand-side exponential to the matching homogeneous exponential.

Invariants
  1. The algebraic formulas themselves remain unchanged while the arrow is added.

Interpretation

The arrow marks the resonance issue: the forcing contains the same exponential factor as one homogeneous solution, motivating the later multiplication by tt in the particular-solution trial.

Grouping terms in the second derivative

Clear evidence
Shown in the video
Evidence
  1. Diagram
    Observation

    A brace is drawn under the parenthetical expression in x¨=Ae−t(−1+t−1)\ddot{x}=Ae^{-t}(-1+t-1) as the speaker comments on combining the terms.

Uncertainties
  1. The simplified result is discussed but not fully rewritten before the clip ends.

Objects
  1. Formula x¨=Ae−t(−1+t−1)\ddot{x}=Ae^{-t}(-1+t-1)

  2. Brace annotation under the parentheses

Changes
  1. A brace is added beneath the grouped terms to emphasize their combination.

Invariants
  1. The prefactor Ae−tAe^{-t} remains outside the grouped expression.

Interpretation

The visual grouping highlights that the bracketed terms should be combined, leading to the simplified factor t−2t-2.

Writing the Substituted Equation

Clear evidence
Shown in the video
Evidence
  1. Animation
    Observation

    The digital pen writes the substituted equation line by line, grouping terms with t and without t.

Objects
  1. Handwritten mathematical expressions on a black background.

Changes
  1. New lines of algebraic expressions appear sequentially as the speaker talks.

  2. Terms are grouped and simplified visually on the board.

Invariants
  1. The original differential equation and trial solution remain visible at the top of the screen.

Interpretation

The visual progression mirrors the algebraic steps of substituting the trial solution into the ODE and collecting like terms to solve for A.

Displaying the Final Particular Solution

Clear evidence
Shown in the video
Evidence
  1. Animation
    Observation

    The speaker writes 'Xp(t)=2X_p(t) = 2te^{-t}' at the bottom of the board.

Objects
  1. The final equation Xp(t)=2X_p(t) = 2te^{-t}.

Changes
  1. The value A=2A=2 is substituted into the general trial form to produce the specific particular solution.

Invariants
  1. The structure of the trial solution x = Ate^{-t} remains the same, only the constant A is fixed.

Interpretation

This visual event concludes the derivation by presenting the explicit formula for the particular solution.

Whiteboard display of ODE solution

Clear evidence
Shown in the video
Evidence
  1. Diagram
    Observation

    Handwritten mathematical equations on a black background.

Objects
  1. Differential equation

  2. Algebraic substitution steps

  3. Final particular solution

Invariants
  1. The text remains static throughout the 4-second clip.

Interpretation

The visual presents the final algebraic steps of solving for a particular solution using the method of undetermined coefficients.

Misconceptions · 2

Do not use the unmodified guess for resonant forcing

Clear evidence
Shown in the video
Evidence
  1. Audio
    Observation

    The speaker says the complication is that e−te^{-t} is a solution of the homogeneous equation, and therefore the trial particular solution must be multiplied by tt.

  2. Diagram
    Observation

    The arrow from 2e−t2e^{-t} to the e−te^{-t} term in xh(t)x_h(t) visually marks the overlap.

Misconception

One might try a particular solution of the form Ae−tAe^{-t} directly because the right-hand side is proportional to e−te^{-t}.

Clarification

The video shows that this fails in the resonant case because e−te^{-t} already belongs to the homogeneous solution, so the correct trial is Ate−tAte^{-t}.

Resonance Requires Multiplying by t

Clear evidence
Supplementary explanation
Evidence
  1. Formula
    Observation

    The video explicitly uses x = Ate^{-t} instead of x = Ae^{-t} for the particular solution.

Misconception

Students might incorrectly guess the particular solution as x = Ae^{-t} when the forcing term e−te^{-t} is already part of the homogeneous solution.

Clarification

When there is resonance (the forcing exponent matches a root of the characteristic equation), the trial solution must be multiplied by t to ensure linear independence from the homogeneous solutions.

Concept relations · 8

Nonhomogeneous second-order linear ODE with exponential forcing → Characteristic-equation method for the homogeneous ODE

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    The board moves from the nonhomogeneous ODE to 'hom eq: Try x=ex=e^{rt}'.

Prerequisite
Explanation

The particular-solution discussion depends on first understanding the associated homogeneous equation and its characteristic roots.

Characteristic-equation method for the homogeneous ODE → Homogeneous solution and overlap with the forcing term

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    The factorization (r+2)(r+1)=0(r+2)(r+1)=0 is followed by the displayed solution xh(t)=c1e−2t+c2e−tx_h(t)=c_1e^{-2t}+c_2e^{-t}.

Proof dependency
Explanation

The homogeneous solution is derived directly from the roots found by the characteristic-equation method.

Homogeneous solution and overlap with the forcing term → Resonance-adjusted trial for the particular solution

Clear evidence
Shown in the video
Evidence
  1. Diagram
    Observation

    An arrow connects the forcing term 2e−t2e^{-t} to the e−te^{-t} component of the homogeneous solution.

  2. Audio
    Observation

    The speaker explains that this overlap forces multiplication by tt in the particular-solution trial.

Prerequisite
Explanation

Recognizing that e−te^{-t} is a homogeneous mode is what motivates the resonant ansatz Ate−tAte^{-t}.

Resonance-adjusted trial for the particular solution → First derivative of the resonant trial solution

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    After writing x=Ate−tx=Ate^{-t}, the board successively computes x˙\dot{x} and x¨\ddot{x}.

Application
Explanation

The chosen trial solution is then differentiated so it can be substituted into the differential equation.

First derivative of the resonant trial solution → Second derivative of the resonant trial solution

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    The second derivative is computed from the previously written first derivative Ae−t(1−t)Ae^{-t}(1-t).

Proof dependency
Explanation

The second-derivative calculation depends directly on the already obtained first derivative.

Trial Particular Solution Form → Substituting Trial Solution into ODE

Clear evidence
Shown in the video
Evidence
  1. Audio
    Observation

    The speaker transitions from stating the trial solution to saying 'So we substitute into the differential equation'.

Application
Explanation

The chosen trial solution form is directly applied in the substitution step to evaluate the left-hand side of the ODE.

Substituting Trial Solution into ODE → Collecting Like Terms After Substitution

Clear evidence
Shown in the video
Evidence
  1. Audio
    Observation

    The speaker says, 'So we collect the terms,' immediately after writing the substituted expression.

Application
Explanation

After substitution, the resulting complex expression must be collected and simplified to isolate the undetermined coefficient.

Method of Undetermined Coefficients → Second-order linear non-homogeneous ODE

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    The method is applied directly to the displayed ODE.

Application
Explanation

The Method of Undetermined Coefficients is the technique being used to solve the specific second-order linear non-homogeneous ODE shown.

Find an answer · 7

Why does the particular solution use Ate−tAte^{-t} instead of Ae−tAe^{-t}?

Clear evidence
Shown in the video
Evidence
  1. Audio
    Observation

    The speaker explicitly says the complication is that e−te^{-t} solves the homogeneous equation and therefore the right-hand side must be multiplied by tt.

  2. Diagram
    Observation

    The arrow annotation links the forcing term to the homogeneous mode.

Knowledge points
  1. Homogeneous solution and overlap with the forcing term
  2. Resonance-adjusted trial for the particular solution
  3. Do not use the unmodified guess for resonant forcing

How are the homogeneous roots r=−2r=-2 and r=−1r=-1 obtained for this ODE?

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    The board shows r2+3r+2=0⇒(r+2)(r+1)=0r^2+3r+2=0\Rightarrow(r+2)(r+1)=0 and then xh(t)=c1e−2t+c2e−tx_h(t)=c_1e^{-2t}+c_2e^{-t}.

Knowledge points
  1. Characteristic-equation method for the homogeneous ODE
  2. Homogeneous solution and overlap with the forcing term

What are the first and second derivatives of the resonant trial solution Ate−tAte^{-t}?

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    The board displays x˙=Ae−t(1−t)\dot{x}=Ae^{-t}(1-t) and x¨=Ae−t(−1+t−1)\ddot{x}=Ae^{-t}(-1+t-1).

  2. Audio
    Observation

    The speaker verbally applies the product rule twice.

Uncertainties
  1. The final simplification of the second derivative is not fully written before the clip ends.

Knowledge points
  1. First derivative of the resonant trial solution
  2. Second derivative of the resonant trial solution

Where does this segment stop in the method of undetermined coefficients?

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    The clip ends after computing derivatives but before substituting them into the ODE.

Uncertainties
  1. The value of A is absent from this segment.

Knowledge points
  1. Second derivative of the resonant trial solution
  2. Worked example: particular solution setup for x¨+3x˙+2x=2e−t\ddot{x}+3\dot{x}+2x=2e^{-t}

Why do we multiply by t in the trial solution for a resonant ODE?

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    The board shows 'Try x = Ate^{-t}' for the particular solution.

Knowledge points
  1. Trial Particular Solution Form

How do you find the coefficient A in the method of undetermined coefficients?

Clear evidence
Shown in the video
Evidence
  1. Formula
    Observation

    The derivation shows how substituting the trial solution leads to the equation A=2A = 2.

Knowledge points
  1. Substituting Trial Solution into ODE
  2. Collecting Like Terms After Substitution

How do you find the particular solution for a second-order ODE with resonance?

Clear evidence
Supplementary explanation
Evidence
  1. Formula
    Observation

    xp(t)=2x_p(t) = 2te^{-t}

Knowledge points
  1. Second-order linear non-homogeneous ODE
  2. Method of Undetermined Coefficients
Coverage and review notes

Covered · The ODE is displayed and the goal of finding a particular solution is stated.

Covered · The homogeneous trial x=ertx=e^{rt} and characteristic equation are written and factored.

Covered · The homogeneous solution is displayed and the resonance with e−te^{-t} is marked by an arrow.

Covered · The speaker introduces the modified particular-solution trial Ate−tAte^{-t}.

Covered · The first derivative of the trial solution is computed using the product rule.

Covered · The second derivative is computed in unsimplified form and grouped visually; the clip ends before substitution and solving for A.

Covered · Introduction of the resonant trial solution x = Ate^{-t} and its derivatives.

Covered · Substitution into the ODE, algebraic simplification, and solving for A=2A = 2.

Covered · Writing the final particular solution Xp(t)=2X_p(t) = 2te^{-t}.

Covered · The entire 4-second clip shows a static whiteboard with the final steps of solving an ODE.

Explore the knowledge in this video

Open video knowledge graph →

  • Resonance ExplanationAt 0:00
    Why this connection?

    Reviewed English material v1: card "Resonance in a second-order linear ODE" at 0:00 — For x¨+3x˙+2x=2e−t\ddot{x}+3\dot{x}+2x=2e^{-t}, the forcing exponential e−te^{-t} is not independent of the homogeneous solution. The video first solves the homogeneous equation and finds xh(t)=c1e−2t+c2e−tx_h(t)=c_1e^{-2t}+c_2e^{-t}, so e−te^{-t} is already present. That overlap is the reason the particular-solution trial must be modified.

  • Characteristic equations ExplanationAt 0:23
    Why this connection?

    Reviewed English material v1: card "Characteristic equation from the exponential trial" at 0:23 — Trying x=ertx=e^{rt} in the homogeneous equation produces r2+3r+2=0r^2+3r+2=0, which factors as (r+2)(r+1)=0(r+2)(r+1)=0. Hence the roots are r=−2r=-2 and r=−1r=-1, giving the two homogeneous modes e−2te^{-2t} and e−te^{-t}.

  • Undetermined coefficients ExplanationAt 5:30
    Why this connection?

    Reviewed explanation connection to Undetermined coefficients.

Questions this video answers

Understand why

↗
Find a method

↗
Find a method

↗
Meet the concept

↗
Meet the concept

↗
Know when to use it

↗