Main derivation
S01 · definition
Before
\text{linear harmonic oscillator}After
mx''+kx=0,\ m>0,\ k>0
Conditions: m>0; k>0
Rule: mko_sho · Uses: G1, mko_sho
Leaf basis: mko_sho + def_intro
Fix the model as the MKO states it: positive mass m, positive spring coefficient k, and displacement x satisfying m x''+k x=0. The MKO is explicit that k/m is only called the angular-frequency-square candidate, and that a general closed form needs separately established trigonometric and derivative semantics, which this guide does not use.
S02 · implies
Before
(m,k)=(2,8)
After
m>0\land k>0:\ \text{qualifies};\ (0,8),\ (2,-8)\ \text{do not}Conditions: none
Rule: and_intro_elim · Uses: S01, G1, G4
Leaf basis: and_intro_elim + de_morgan_logic + order_basics
Eligibility is the conjunction m>0 and k>0. Both hold for (2,8), so it qualifies. Non-instances: (0,8) has m=0, which is not positive; (2,−8) has k=−8<0. Neither belongs to this model, even though both can be written in the form m x''+k x=0 (with m=0 it is no longer even a second-order equation).
S03 · equivalent
Before
\tfrac{k}{m}After
\tfrac{8}{2}=4Conditions: m\neq 0
Rule: numeric_evaluation · Uses: S02, mko_sho
Leaf basis: numeric_evaluation + frac_rules
k/m=8/2=4, and m≠0 allows the division. By the MKO, 4 is called only the angular-frequency-square candidate; reading it as 'angular frequency 2' or as a 'frequency' needs trigonometric semantics, which this guide does not supply.
S04 · equivalent
Before
x_c(t)=1-2t^2
After
x_c'(t)=-4t,\ x_c''(t)=-4
Conditions: none
Rule: poly_deriv · Uses: G2, poly_deriv
Leaf basis: poly_deriv + numeric_evaluation
(1)'=0 and (−2t²)'=−2·2t=−4t; differentiating again, (−4t)'=−4. Cross-check: x_c(t+h)−x_c(t)=−4t·h−2h² (N10, a polynomial identity); dividing by h and letting h→0 gives −4t.
S05 · equivalent
Before
R(t)=m x_c''(t)+k x_c(t)
After
R(t)=-16t^2
Conditions: none
Rule: distributive · Uses: S04, G1
Leaf basis: eq_replace + distributive
Substitute m=2, k=8 and the derivatives of S04, then expand and simplify (sub-step S05.1). The residual is the polynomial −16t², with a definite value for every t.
S06 · equivalent
Before
t\in\{0,\tfrac{1}{2},1\}After
R(0)=0,\ R(\tfrac{1}{2})=-4,\ R(1)=-16Conditions: none
Rule: numeric_evaluation · Uses: S05, G2
Leaf basis: numeric_evaluation
Evaluate the residual at the specified points: R(0)=0, R(1/2)=−16·1/4=−4 and R(1)=−16 (N3, N4). Only at t=0 is the residual zero.
S07 · implies
Before
R(t)=-16t^2
After
x_c\ \text{solves the equation on no interval of positive length}Conditions: none
Rule: quantifier_negation · Uses: S05, S06, quantifier_negation
Leaf basis: quantifier_negation + square_nonneg + order_basics
For t≠0, t²>0, so R(t)=−16t²<0≠0. Every interval of positive length contains a point t≠0, where the residual is nonzero, so 'R(t)=0 for every t in the interval' fails. R(0)=0 is a single-point fact and cannot make x_c a solution.
S08 · implies
Before
x\ \text{polynomial},\ 2x''+8x=0\ \text{on an interval}After
x=0
Conditions: m\neq 0; k\neq 0
Rule: L_no_poly · Uses: G1, poly_deriv, poly_roots
Leaf basis: contradiction + poly_deriv + poly_roots + zero_product
Prove Lemma L_no_poly: this equation has no nonzero polynomial solution. This shows that the failure in S07 is not a matter of choosing the wrong coefficients: no polynomial candidate other than zero can be a solution, and nonzero solutions must come from non-polynomial functions, such as trigonometric functions whose semantics must be established separately. Three sub-steps reach a contradiction by comparing leading coefficients.
S09 · implies
Before
\text{nonzero solution}\ xAfter
x\ \text{is not a polynomial}Conditions: none
Rule: contrapositive · Uses: S03, S08, mko_sho
Leaf basis: contrapositive + mko_sho
The contrapositive of L_no_poly: a nonzero solution is not a polynomial. The MKO says a general closed form needs separately established trigonometric and derivative semantics; this guide establishes neither, so it claims no specific formula for a nonzero solution and does not even claim that one exists.
S10 · equivalent
Before
E(1,0)
After
\tfrac{2\cdot 0^2}{2}+\tfrac{8\cdot 1^2}{2}=4Conditions: none
Rule: numeric_evaluation · Uses: G3, G1
Leaf basis: numeric_evaluation
By the MKO, the energy expression can be used as a single-state quantity: E(1,0)=2·0/2+8·1/2=4 (N5). It is one number for one state and involves no evolution in time.
S11 · equivalent
Before
E(t)=E(x_c(t),x_c'(t))
After
E(t)=16t^2+4(1-2t^2)^2=4+16t^4
Conditions: none
Rule: distributive · Uses: S04, G3, G1
Leaf basis: distributive + power_laws + numeric_evaluation
Compute the energy along the candidate x_c: m x_c'²/2=(2/2)(16t²)=16t² and k x_c²/2=4(1−4t²+4t⁴)=4−16t²+16t⁴; the sum is E(t)=4+16t⁴ (N6). So E(0)=4 (the same state (1,0) as in S10), but E(1)=20 (N7): along this non-solution curve the energy is not constant.
S12 · implies
Before
E(t)=\tfrac{m}{2}x'(t)^2+\tfrac{k}{2}x(t)^2After
E'(t)=x'(t)\big(mx''(t)+kx(t)\big)
Conditions: x\ \text{twice differentiable}
Rule: L_energy · Uses: mko_deriv_rules
Leaf basis: mko_deriv_rules
Prove Lemma L_energy: along any twice-differentiable curve, the rate of change of the energy equals the velocity times the residual. An identically zero residual is sufficient for E' to vanish identically; the converse generally fails because the product can also vanish when the velocity is zero. One energy value provides no such interval-wide information.
S13 · implies
Before
x_c'(t)R(t)=(-4t)(-16t^2)
After
64t^3=\tfrac{d}{dt}(4+16t^4)Conditions: none
Rule: L_energy · Uses: S05, S11, S12, S04
Leaf basis: L_energy + poly_deriv + numeric_evaluation
Check the lemma on the candidate: x_c'·R=(−4t)(−16t²)=64t³ (N8), and the derivative of E(t)=4+16t⁴ from S11 is 64t³ (N9 checks this through a difference-quotient identity); they agree. The change in energy comes exactly from the nonzero residual. For a genuine solution the residual is identically zero, so E'(t)=0 at every point; concluding that E is constant would further need the theorem that a function with zero derivative on an interval is constant, which this guide does not use. The single-state value E=4 proves no conservation.
S14 · implies
Before
m=2,\ k=8,\ x_c=1-2t^2,\ (x,v)=(1,0)
After
\text{qualifies};\ \tfrac{k}{m}=4;\ x_c\ \text{not a solution};\ \text{no nonzero polynomial solution};\ E(1,0)=4Conditions: none
Rule: and_intro_elim · Uses: S02, S03, S07, S08, S10, S13
Leaf basis: and_intro_elim
Summary: (2,8) qualifies (S02) and k/m=4 is the angular-frequency-square candidate (S03); x_c has zero residual only at t=0 and solves the equation on no interval of positive length (S06, S07); there is no nonzero polynomial solution (S08); the single-state energy is E(1,0)=4 (S10), and for a genuine solution the identically zero residual makes E' identically zero (S12, S13), a sufficient direction. A single energy value proves no conservation, and E'≡0 alone does not imply a zero residual.
Substeps and lemmas
S05.1 · equivalent
Before
2\cdot(-4)+8(1-2t^2)
After
-8+8-16t^2=-16t^2
Conditions: none
Rule: distributive · Uses: S04, G1, distributive
Leaf basis: distributive + add_inverse + add_zero
2·(−4)=−8; 8(1−2t²)=8−16t² by distributivity; −8+8=0, leaving −16t².
S08.1 · implies
Before
x(t)=\sum_{j=0}^{d}a_jt^j,\ a_d\neq 0After
[t^d]\,(kx)=k\,a_d\neq 0
Conditions: k\neq 0; a_d\neq 0
Rule: zero_product · Uses: poly_deriv, zero_product
Leaf basis: zero_product + distributive
Suppose, for contradiction, that x is not the zero polynomial, with degree d and leading coefficient a_d≠0. The t^d coefficient of k x is k a_d; since k≠0 and a_d≠0, the zero-product property gives k a_d≠0.
S08.2 · implies
Before
x\ \text{of degree}\ dAfter
[t^d]\,(mx'')=0
Conditions: none
Rule: poly_deriv · Uses: S08.1, poly_deriv
Leaf basis: poly_deriv + case_analysis
If d≤1, x'' is the zero polynomial and m x''=0; if d≥2, differentiating twice lowers the degree to d−2<d, so m x'' has no t^d term. In both cases the t^d coefficient of m x'' is 0.
S08.3 · implies
Before
[t^d]\,(mx''+kx)=0+k\,a_d\neq 0
After
mx''+kx\neq 0\ \text{on any interval}\ \Rightarrow\ \botConditions: none
Rule: contradiction · Uses: S08.1, S08.2, poly_roots
Leaf basis: contradiction + poly_roots + add_assoc
Adding polynomials adds coefficients of equal degree, so the t^d coefficient of m x''+k x is 0+k a_d≠0; it is a nonzero polynomial with at most d roots and cannot vanish everywhere on an interval of positive length. This contradicts 'x solves the equation on that interval', so x is the zero polynomial. S08.1 to S08.3 prove Lemma L_no_poly.
S12.1 · equivalent
Before
\big(\tfrac{m}{2}x'^2+\tfrac{k}{2}x^2\big)'After
\tfrac{m}{2}\cdot 2x'x''+\tfrac{k}{2}\cdot 2xx'=x'(mx''+kx)Conditions: x\ \text{twice differentiable}
Rule: mko_deriv_rules · Uses: mko_deriv_rules
Leaf basis: mko_deriv_rules + distributive + mul_comm
Differentiate term by term with the sum and constant-multiple rules; by the product rule, (x'·x')'=x''x'+x'x''=2x'x'' and (x·x)'=2xx'. So E'=(m/2)·2x'x''+(k/2)·2xx'=m x'x''+k x x'=x'(m x''+k x) by distributivity. This proves Lemma L_energy.