Reviewed learning material · Video analysis · EnglishRead the full overview
This whiteboard segment works on the nonhomogeneous ODE x¨+3x˙+2x=2e−t and focuses on the resonance issue in the method of undetermined coefficients. The presenter first solves the homogeneous equation via x=ert, obtaining (r+2)(r+1)=0 and hence xh(t)=c1e−2t+c2e−t. Because the forcing term contains e−t, the video explicitly shows that the naive particular guess must be multiplied by t, leading to the trial xp(t)=Ate−t. The remainder of the clip computes x˙p=Ae−t(1−t) and x¨p=Ae−t(−1+t−1)=Ae−t(t−2), stopping before substitution into the ODE and before determining the constant A.
This segment demonstrates finding a particular solution to the non-homogeneous ODE x¨+3x˙+2x=2e−t using the method of undetermined coefficients. Because the forcing term e−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−t, collects like terms, and solves for the coefficient A=2, yielding the final particular solution Xp(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 is solved by substituting an assumed form, leading to the coefficient A=2 and the final particular solution xp(t)=2te^{-t}.
Use the learning inspector for key ideas and moments, or open the reading tabs for the complete notes.
Generated from the video's visuals and explanation; not verbatim speech.
The clip opens on the equation x¨+3x˙+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−t may already belong to the homogeneous solution space.
Using the standard exponential trial x=ert, the homogeneous equation leads to the characteristic polynomial r2+3r+2=0, which factors as (r+2)(r+1)=0.
Therefore the complementary solution is xh(t)=c1e−2t+c2e−t. The board then visually links the forcing term 2e−t to the homogeneous mode e−t, showing the resonance problem.
Because of that overlap, the usual non-resonant guess Ae−t is replaced by the modified ansatz xp(t)=Ate−t, where A 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).
Differentiating once more gives x¨p=Ae−t(−1+t−1), which simplifies to Ae−t(t−2). The segment stops here, before substituting these expressions back into the differential equation and solving for A.
We begin with the trial particular solution x=Ate−t, chosen because the forcing term e−t causes resonance with the homogeneous solution. Its derivatives are x˙=Ae−t(1−t) and x¨=Ae−t(−2+t).
Next, we substitute these expressions into the left-hand side of the differential equation x¨+3x˙+2x. This gives Ae−t(−2+t)+3Ae−t(1−t)+2Ate−t=2e−t.
Since e−t is never zero, we can divide both sides by e−t to simplify the equation to A(−2+t)+3A(1−t)+2At=2.
Now we collect like terms. The terms proportional to t are At−3At+2At, which sum to 0t and cancel out completely. The constant terms are −2A+3A, which simplify to A.
Equating the remaining constant term to the right-hand side gives A=2. Substituting this back into our initial guess, we find the particular solution is Xp(t)=2te−t.
The whiteboard displays the differential equation x¨+3x˙+2x=2. Below it, the substitution step is shown as (A−3A+2A)t+(−2A+3A)=2, which simplifies to yield A=2. The final particular solution is written at the bottom as xp(t)=2te−t.
Knowledge cards
01
Resonance in a second-order linear ODE
For x¨+3x˙+2x=2e−t, the forcing exponential e−t is not independent of the homogeneous solution. The video first solves the homogeneous equation and finds xh(t)=c1e−2t+c2e−t, so e−t is already present. That overlap is the reason the particular-solution trial must be modified.
x¨+3x˙+2x=2e−t
02
Characteristic equation from the exponential trial
Trying x=ert in the homogeneous equation produces r2+3r+2=0, which factors as (r+2)(r+1)=0. Hence the roots are r=−2 and r=−1, giving the two homogeneous modes e−2t and e−t.
x=ert⇒r2+3r+2=0⇒(r+2)(r+1)=0
03
Why the particular guess becomes Ate−t
In the method of undetermined coefficients, if the forcing term duplicates a homogeneous solution, the naive guess must be multiplied by t. Here the duplicate mode is e−t, so the correct trial is xp(t)=Ate−t rather than Ae−t.
xp(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). Second, 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 A, but that final step is not shown in this segment.
x˙p=Ae−t(1−t),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 t. Here, since e−t is in the homogeneous solution, the trial particular solution is x=Ate−t rather than x=Ae−t.
x=Ate−t
06
Substituting into the ODE
To find the undetermined coefficient A, substitute the trial solution and its derivatives into the original differential equation. For x¨+3x˙+2x=2e−t, using x=Ate−t, x˙=Ae−t(1−t), and x¨=Ae−t(−2+t) leads to an equation where e−t can be canceled from all terms.
Ae−t(−2+t)+3Ae−t(1−t)+2Ate−t=2e−t
07
Collecting Terms and Solving for A
After canceling e−t, expand and group the remaining expression by powers of t. The coefficients of t 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 A. In this example, −2A+3A=2 yields A=2.
(A−3A+2A)t+(−2A+3A)=2⟹A=2
08
Final Particular Solution
Once the coefficient A is determined, substitute it back into the trial form to state the final particular solution. With A=2, the particular solution for the given ODE is Xp(t)=2te−t.
Xp(t)=2te−t
09
Particular Solution via Undetermined Coefficients
To solve the non-homogeneous ODE x¨+3x˙+2x=2, we assume a particular solution form and substitute it into the equation. Grouping the terms by powers of t gives (A−3A+2A)t+(−2A+3A)=2. The coefficient of t becomes 0, and the constant term becomes A. Setting A=2 allows us to write the final particular solution as xp(t)=2te−t.
xp(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
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
Formula
Observation
The independent variable appears as t in e−t, e^{rt}, and the trial particular solution Ate−t.
Symbol
t
Meaning
Independent variable (time-like parameter) of the ODE.
Domain
Real variable; no explicit interval is shown.
x˙
Clear evidence
Shown in the video
Evidence
Formula
Observation
The first derivative is written as x˙ in the ODE and later computed explicitly.
Symbol
x˙
Meaning
First derivative of x with respect to t.
Domain
Defined wherever x is differentiable.
x¨
Clear evidence
Shown in the video
Evidence
Formula
Observation
The second derivative is written as x¨ in the ODE and later computed explicitly.
Symbol
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
Formula
Observation
r appears in the trial homogeneous solution x=e^{rt} and in the characteristic polynomial r2+3r+2=0.
Symbol
r
Meaning
Exponential rate parameter used in the homogeneous trial solution.
Domain
Algebraic unknown solved from the characteristic equation.
c1
Clear evidence
Shown in the video
Evidence
Formula
Observation
c1 multiplies e−2t in the displayed homogeneous solution.
Symbol
c1
Meaning
Arbitrary constant multiplying the homogeneous mode e−2t.
Domain
Constant of integration; numerical value not specified.
c2
Clear evidence
Shown in the video
Evidence
Formula
Observation
c2 multiplies e−t in the displayed homogeneous solution.
Symbol
c2
Meaning
Arbitrary constant multiplying the homogeneous mode e−t.
Domain
Constant of integration; numerical value not specified.
A
Clear evidence
Shown in the video
Evidence
Formula
Observation
A is introduced as the unknown coefficient in the trial particular solution x=Ate−t.
Uncertainties
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
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
Formula
Observation
The variable t appears as the independent variable in e−t and te^{-t}.
Symbol
t
Meaning
Independent variable (time).
Domain
Real numbers.
A
Clear evidence
Shown in the video
Evidence
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˙
Clear evidence
Shown in the video
Evidence
Formula
Observation
The notation x˙ appears in the differential equation and its derivative expression.
Symbol
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
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.
Formula
Observation
The board shows x¨+3x˙+2x=2e−t.
Definition
Explanation
The clip studies the differential equation x¨+3x˙+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
Conditions
Linear second-order ODE with constant coefficients.
Right-hand side is 2e−t.
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
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'.
Formula
Observation
The board writes 'hom eq: Try x=e^{rt}' and then 'r2+3r+2=0 => (r+2)(r+1)=0'.
Method
Explanation
To solve the associated homogeneous equation, the video uses the standard exponential trial x=ert. Substitution produces the characteristic polynomial r2+3r+2=0, which factors as (r+2)(r+1)=0. This identifies the two homogeneous exponents r=−2 and r=−1.
Formula
x=ert⇒r2+3r+2=0⇒(r+2)(r+1)=0
Conditions
Applies to the homogeneous equation associated with constant-coefficient linear ODEs.
Distinct real roots are obtained here.
Prerequisites
Nonhomogeneous second-order linear ODE with exponential forcing
Homogeneous solution and overlap with the forcing term
Clear evidence
Shown in the video
Evidence
Audio
Observation
The speaker states the homogeneous solution is some constant times e−2t plus another constant times e−t.
Formula
Observation
The board displays xh(t)=c1e−2t+c2e−t.
Diagram
Observation
An arrow is drawn from the forcing term 2e−t toward the e−t term in the homogeneous solution.
Formula
Explanation
From the roots r=−2 and r=−1, the homogeneous solution is written as xh(t)=c1e−2t+c2e−t. The visual arrow emphasizes that the forcing term 2e−t shares the same exponential factor as one homogeneous mode, so the usual non-resonant guess would fail.
Formula
xh(t)=c1e−2t+c2e−t
Conditions
Roots of the characteristic equation are distinct and real.
This is the complementary solution of the homogeneous ODE.
Prerequisites
Characteristic-equation method for the homogeneous ODE
Resonance-adjusted trial for the particular solution
Clear evidence
Shown in the video
Evidence
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−t.
Formula
Observation
The board writes 'Part sol: Try x=Ate−t'.
Method
Explanation
Because e−t already solves the homogeneous equation, the video modifies the usual undetermined-coefficients guess by multiplying by t. The chosen ansatz is xp(t)=Ate−t, where A is the unknown coefficient to be determined after substitution into the ODE.
Formula
xp(t)=Ate−t
Conditions
Use when the forcing term overlaps a homogeneous solution mode.
Here the overlap is with e−t, so one factor of t is inserted.
Prerequisites
Homogeneous solution and overlap with the forcing term
First derivative of the resonant trial solution
Clear evidence
Shown in the video
Evidence
Audio
Observation
The speaker verbally applies the product rule: derivative of the first times the second plus the first times derivative of the second.
Formula
Observation
The board shows x˙=Ae^{-t}(1-t).
Formula
Explanation
Differentiating x=Ate−t with the product rule gives 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)
Conditions
Differentiate with respect to t.
Product rule applied to t and e−t.
Prerequisites
Resonance-adjusted trial for the particular solution
Second derivative of the resonant trial solution
Clear evidence
Shown in the video
Evidence
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.
Formula
Observation
The board shows x¨=Ae^{-t}(-1+t-1).
Diagram
Observation
A brace groups the terms inside the parentheses as the speaker comments on the combination.
Uncertainties
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) once more yields x¨=Ae−t(−1+t−1). The bracketed terms combine to t−2, so the simplified form is 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)
Conditions
Continue from the previously computed first derivative.
Product rule applied again to e−t and (1−t).
Prerequisites
First derivative of the resonant trial solution
Trial Particular Solution Form
Clear evidence
Shown in the video
Evidence
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−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−t
Conditions
The forcing term contains e−t.
-1 is a simple root of the homogeneous characteristic equation.
Substituting Trial Solution into ODE
Clear evidence
Shown in the video
Evidence
Audio
Observation
The speaker says, 'So we substitute into the differential equation, so x double dot plus 3x dot plus 2x.'
Formula
Observation
The left-hand side operator x¨+3x˙+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
Conditions
x, x˙, and x¨ are evaluated using the trial form x = Ate^{-t}.
Prerequisites
Trial Particular Solution Form
Collecting Like Terms After Substitution
Clear evidence
Shown in the video
Evidence
Audio
Observation
The speaker explains collecting terms proportional to t and terms not proportional to t after canceling e−t.
Formula
Observation
The board shows the grouped expression (A−3A+2A)t+(−2A+3A).
Method
Explanation
After substituting the trial solution and factoring out e−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)
Conditions
The common factor e−t has been canceled from both sides.
Prerequisites
Substituting Trial Solution into ODE
Second-order linear non-homogeneous ODE
Clear evidence
Shown in the video
Evidence
Formula
Observation
x¨+3x˙+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
Conditions
The equation is linear.
The coefficients are constants (1, 3, 2).
The right-hand side is a constant (2).
Method of Undetermined Coefficients
Clear evidence
Shown in the video
Evidence
Formula
Observation
Substitution of terms involving A into the ODE to solve for A.
Uncertainties
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
Applies to linear ODEs with constant coefficients.
The non-homogeneous term must be of a specific type (e.g., polynomial, exponential, sine/cosine).
Prerequisites
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
Audio
Observation
The speaker says the complication is that e−t is a solution of the homogeneous equation.
Formula
Observation
The homogeneous solution contains the term c2e−t.
Diagram
Observation
An arrow visually links the forcing term 2e−t to the e−t part of xh(t).
Proposition
Statement
For the ODE x¨+3x˙+2x=2e−t, the forcing factor e−t belongs to the homogeneous solution space because r=−1 is a root of the characteristic equation.
Hypotheses
Consider the associated homogeneous equation x¨+3x˙+2x=0.
Use the exponential trial x=ert.
The characteristic equation is r2+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
Audio
Observation
The speaker says they need to multiply now the right hand side by t, giving Ate−t.
Formula
Observation
The board writes Part sol: Try x=Ate−t.
Uncertainties
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 t; here the chosen form is xp(t)=Ate−t.
Hypotheses
The ODE is linear with constant coefficients.
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
Audio
Observation
The speaker says trying x=e^{rt} gives the characteristic equation r2+3r+2=0, which factors to (r+2)(r+1)=0.
Formula
Observation
The board shows hom eq: Try x=e^{rt}, then r2+3r+2=0 => (r+2)(r+1)=0.
Proof
Steps
Expression
x¨+3x˙+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
Expression
x=ert
Explanation
Try an exponential solution.
Justification
Standard method for constant-coefficient linear ODEs, as stated in the video.
Shown in the video
Expression
r2+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
Expression
(r+2)(r+1)=0
Explanation
Factor the quadratic.
Justification
Algebraic factorization shown on the board.
Shown in the video
Expression
r=−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=−2 and r=−1, leading to the complementary solution built from e−2t and e−t.
Differentiation of the resonant trial solution
Clear evidence
Shown in the video
Evidence
Audio
Observation
The speaker verbally computes the first and second derivatives using the product rule.
Formula
Observation
The board writes x=Ate^{-t}, then x˙=Ae^{-t}(1-t), then x¨=Ae^{-t}(-1+t-1).
Uncertainties
The clip stops before substituting these derivatives back into the ODE and solving for A.
Proof
Steps
Expression
x=Ate−t
Explanation
Begin with the chosen particular-solution ansatz.
Justification
Selected because e−t overlaps the homogeneous solution.
Shown in the video
Expression
x˙=Ae−t−Ate−t
Explanation
Apply the product rule to t and e−t.
Justification
Speaker explicitly describes derivative of the first times the second plus the first times derivative of the second.
Shown in the video
Expression
x˙=Ae−t(1−t)
Explanation
Factor out Ae−t.
Justification
Algebraic simplification shown on the board.
Shown in the video
Expression
x¨=Ae−t(−1)+(Ae−t)(−1)+A(−e−t)(1−t)
Explanation
Differentiate 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
Expression
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
Expression
x¨=Ae−t(t−2)
Explanation
Simplify the bracket.
Justification
Arithmetic simplification of −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) and 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
Formula
Observation
The board displays the step-by-step substitution and simplification leading to A=2.
Audio
Observation
The speaker narrates the cancellation of the t-proportional terms and the solving of the remaining equation.
Proof
Steps
Expression
x¨+3x˙+2x=2e−t
Explanation
Start with the original non-homogeneous differential equation.
Justification
Given problem statement visible on the board.
Shown in the video
Expression
x=Ate−t,x˙=Ae−t(1−t),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
Expression
Ae−t(−2+t)+3Ae−t(1−t)+2Ate−t=2e−t
Explanation
Substitute x, x˙, and x¨ into the left-hand side of the ODE.
Justification
Direct algebraic substitution.
Shown in the video
Expression
e−t[A(−2+t)+3A(1−t)+2At]=2e−t
Explanation
Factor out the common exponential term e−t.
Justification
Distributive property of multiplication over addition.
Derived from the video
Expression
A(−2+t)+3A(1−t)+2At=2
Explanation
Divide both sides by e−t (which is never zero) to simplify the equation.
Justification
Algebraic cancellation of a non-zero common factor.
Shown in the video
Expression
(A−3A+2A)t+(−2A+3A)=2
Explanation
Expand and collect terms by powers of t.
Justification
Polynomial grouping.
Shown in the video
Expression
0⋅t+A=2
Explanation
Simplify the coefficients: A−3A+2A=0 and -2A + 3A=A.
Justification
Arithmetic simplification.
Shown in the video
Expression
A=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=2.
Solving for the undetermined coefficient A
Clear evidence
Shown in the video
Evidence
Formula
Observation
= (A−3A+2A)t+(−2A+3A)=2⇒A=2
Uncertainties
The initial guess for the particular solution is not shown, but the algebraic steps imply a specific form was substituted.
Proof
Steps
Expression
(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
Expression
0⋅t+A=2
Explanation
The coefficient of t simplifies to zero (A−3A+2A=0), and the constant term simplifies to A(−2A+3A=A).
Justification
Arithmetic calculation.
Derived from the video
Expression
A=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
Clear evidence
Shown in the video
Evidence
Audio
Observation
The entire clip is a worked example of finding a particular solution for the displayed ODE.
Formula
Observation
The board carries the example from the ODE through the homogeneous solution, resonant ansatz, and derivative computations.
Uncertainties
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 when the forcing exponential overlaps a homogeneous solution.
Given
The ODE is x¨+3x˙+2x=2e−t.
The associated homogeneous equation has characteristic polynomial r2+3r+2=0.
The homogeneous solution is xh(t)=c1e−2t+c2e−t.
Goal
Set up the correct resonant trial for a particular solution and compute the derivatives needed for substitution.
Steps
Expression
r2+3r+2=0⇒(r+2)(r+1)=0
Explanation
Solve the homogeneous characteristic equation.
Justification
Shown directly on the board after trying x=ert.
Shown in the video
Expression
xh(t)=c1e−2t+c2e−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
Expression
xp(t)=Ate−t
Explanation
Because e−t is already a homogeneous mode, multiply the naive guess by t.
Justification
Explicitly stated by the speaker as the needed modification for resonance.
Shown in the video
Expression
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
Expression
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−t and computes x˙p=Ae−t(1−t) and x¨p=Ae−t(−1+t−1)=Ae−t(t−2), but it does not reach the final value of A.
Verification
Verification would require substituting xp, x˙p, and x¨p into the original ODE and matching coefficients of e−t; that step is not shown in this segment.
Finding the Particular Solution via Undetermined Coefficients
Clear evidence
Shown in the video
Evidence
Formula
Observation
The entire segment is dedicated to solving for the particular solution of x¨+3x˙+2x=2e−t.
Problem
Find a particular solution to the differential equation x¨+3x˙+2x=2e−t.
Given
The differential equation is x¨+3x˙+2x=2e−t.
The homogeneous solution contains the term e−t, indicating resonance with the forcing function.
Goal
Determine the specific form and coefficient of the particular solution Xp(t).
Steps
Expression
x=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
Expression
x˙=Ae−t(1−t),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
Expression
(A−3A+2A)t+(−2A+3A)=2
Explanation
Substitute into the ODE, cancel e−t, and group like terms.
Justification
Algebraic manipulation and equating coefficients.
Shown in the video
Expression
A=2
Explanation
Solve for the unknown coefficient A.
Justification
Simplifying the grouped equation yields A=2.
Shown in the video
Expression
Xp(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)=2te^{-t}
Verification
Substituting Xp(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
Diagram
Observation
An arrow is drawn from the forcing term 2e−t in the top equation toward the e−t term in the homogeneous solution.
Objects
Top equation x¨+3x˙+2x=2e−t
Homogeneous solution xh(t)=c1e−2t+c2e−t
Arrow annotation
Changes
A new arrow annotation appears connecting the right-hand-side exponential to the matching homogeneous exponential.
Invariants
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 t in the particular-solution trial.
Grouping terms in the second derivative
Clear evidence
Shown in the video
Evidence
Diagram
Observation
A brace is drawn under the parenthetical expression in x¨=Ae−t(−1+t−1) as the speaker comments on combining the terms.
Uncertainties
The simplified result is discussed but not fully rewritten before the clip ends.
Objects
Formula x¨=Ae−t(−1+t−1)
Brace annotation under the parentheses
Changes
A brace is added beneath the grouped terms to emphasize their combination.
Invariants
The prefactor Ae−t remains outside the grouped expression.
Interpretation
The visual grouping highlights that the bracketed terms should be combined, leading to the simplified factor t−2.
Writing the Substituted Equation
Clear evidence
Shown in the video
Evidence
Animation
Observation
The digital pen writes the substituted equation line by line, grouping terms with t and without t.
Objects
Handwritten mathematical expressions on a black background.
Changes
New lines of algebraic expressions appear sequentially as the speaker talks.
Terms are grouped and simplified visually on the board.
Invariants
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
Animation
Observation
The speaker writes 'Xp(t)=2te^{-t}' at the bottom of the board.
Objects
The final equation Xp(t)=2te^{-t}.
Changes
The value A=2 is substituted into the general trial form to produce the specific particular solution.
Invariants
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
Diagram
Observation
Handwritten mathematical equations on a black background.
Objects
Differential equation
Algebraic substitution steps
Final particular solution
Invariants
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
Audio
Observation
The speaker says the complication is that e−t is a solution of the homogeneous equation, and therefore the trial particular solution must be multiplied by t.
Diagram
Observation
The arrow from 2e−t to the e−t term in xh(t) visually marks the overlap.
Misconception
One might try a particular solution of the form Ae−t directly because the right-hand side is proportional to e−t.
Clarification
The video shows that this fails in the resonant case because e−t already belongs to the homogeneous solution, so the correct trial is Ate−t.
Resonance Requires Multiplying by t
Clear evidence
Supplementary explanation
Evidence
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−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
Formula
Observation
The board moves from the nonhomogeneous ODE to 'hom eq: Try x=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
Formula
Observation
The factorization (r+2)(r+1)=0 is followed by the displayed solution xh(t)=c1e−2t+c2e−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
Diagram
Observation
An arrow connects the forcing term 2e−t to the e−t component of the homogeneous solution.
Audio
Observation
The speaker explains that this overlap forces multiplication by t in the particular-solution trial.
Prerequisite
Explanation
Recognizing that e−t is a homogeneous mode is what motivates the resonant ansatz Ate−t.
Resonance-adjusted trial for the particular solution → First derivative of the resonant trial solution
Clear evidence
Shown in the video
Evidence
Formula
Observation
After writing x=Ate−t, the board successively computes x˙ and 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
Formula
Observation
The second derivative is computed from the previously written first derivative 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
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
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
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−t instead of Ae−t?
Clear evidence
Shown in the video
Evidence
Audio
Observation
The speaker explicitly says the complication is that e−t solves the homogeneous equation and therefore the right-hand side must be multiplied by t.
Diagram
Observation
The arrow annotation links the forcing term to the homogeneous mode.
Knowledge points
Homogeneous solution and overlap with the forcing term
Resonance-adjusted trial for the particular solution
Do not use the unmodified guess for resonant forcing
How are the homogeneous roots r=−2 and r=−1 obtained for this ODE?
Clear evidence
Shown in the video
Evidence
Formula
Observation
The board shows r2+3r+2=0⇒(r+2)(r+1)=0 and then xh(t)=c1e−2t+c2e−t.
Knowledge points
Characteristic-equation method for the homogeneous ODE
Homogeneous solution and overlap with the forcing term
What are the first and second derivatives of the resonant trial solution Ate−t?
Clear evidence
Shown in the video
Evidence
Formula
Observation
The board displays x˙=Ae−t(1−t) and x¨=Ae−t(−1+t−1).
Audio
Observation
The speaker verbally applies the product rule twice.
Uncertainties
The final simplification of the second derivative is not fully written before the clip ends.
Knowledge points
First derivative of the resonant trial solution
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
Formula
Observation
The clip ends after computing derivatives but before substituting them into the ODE.
Uncertainties
The value of A is absent from this segment.
Knowledge points
Second derivative of the resonant trial solution
Worked example: particular solution setup for x¨+3x˙+2x=2e−t
Why do we multiply by t in the trial solution for a resonant ODE?
Clear evidence
Shown in the video
Evidence
Formula
Observation
The board shows 'Try x = Ate^{-t}' for the particular solution.
Knowledge points
Trial Particular Solution Form
How do you find the coefficient A in the method of undetermined coefficients?
Clear evidence
Shown in the video
Evidence
Formula
Observation
The derivation shows how substituting the trial solution leads to the equation A=2.
Knowledge points
Substituting Trial Solution into ODE
Collecting Like Terms After Substitution
How do you find the particular solution for a second-order ODE with resonance?
Clear evidence
Supplementary explanation
Evidence
Formula
Observation
xp(t)=2te^{-t}
Knowledge points
Second-order linear non-homogeneous ODE
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=ert and characteristic equation are written and factored.
Covered · The homogeneous solution is displayed and the resonance with e−t is marked by an arrow.
Covered · The speaker introduces the modified particular-solution trial Ate−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=2.
Covered · Writing the final particular solution Xp(t)=2te^{-t}.
Covered · The entire 4-second clip shows a static whiteboard with the final steps of solving an ODE.
Reviewed English material v1: card "Resonance in a second-order linear ODE" at 0:00 — For x¨+3x˙+2x=2e−t, the forcing exponential e−t is not independent of the homogeneous solution. The video first solves the homogeneous equation and finds xh(t)=c1e−2t+c2e−t, so e−t is already present. That overlap is the reason the particular-solution trial must be modified.
Reviewed English material v1: card "Characteristic equation from the exponential trial" at 0:23 — Trying x=ert in the homogeneous equation produces r2+3r+2=0, which factors as (r+2)(r+1)=0. Hence the roots are r=−2 and r=−1, giving the two homogeneous modes e−2t and e−t.
The particular solution uses Ate−t because the forcing term e−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 t to ensure linear independence.
Conditions: The ODE is linear with constant coefficients.; The forcing term contains e−t.; r=−1 is a root of the homogeneous characteristic equation.
The homogeneous roots are obtained by solving the associated homogeneous equation x¨+3x˙+2x=0. By substituting the exponential trial solution x=ert, the differential equation converts into the characteristic polynomial r2+3r+2=0, which factors to (r+2)(r+1)=0, yielding the roots r=−2 and r=−1.
Conditions: The ODE has constant coefficients.; The trial solution is of the form x=ert.; The characteristic equation is a quadratic polynomial.
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 x¨+3x˙+2x=2e−t.; e−t is never zero, allowing it to be canceled from both sides.
The first derivative is x˙=Ae−t(1−t), and the second derivative is x¨=Ae−t(t−2). These are computed by applying the product rule successively to the trial solution x=Ate−t.
Conditions: The trial solution is x=Ate−t.; Differentiation is with respect to t.; The product rule is applied to t and e−t.
The final particular solution is Xp(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 x¨+3x˙+2x=2e−t.; The coefficient A has been determined to be 2.; The trial solution form is x=Ate−t.
The first segment stops after computing the first and second derivatives of the resonant trial solution x=Ate−t. It does not yet substitute these derivatives back into the differential equation or solve for the unknown coefficient A.
Conditions: The segment covers the setup of the homogeneous solution and the resonant trial solution.; The derivatives x˙ and x¨ are computed but not substituted.