Form the auxiliary equation
m2−m−6=0 Trying un=mn turns the homogeneous model into this quadratic.
Solve for the roots
m=−2, m=3 The roots decide the shape of the general solution.
Match the roots to the correct solution shape
un=A⋅3n+B(−2)n Two distinct real roots give two independent geometric terms.
Reject options using the coefficients as roots
coefficients are not the roots of the auxiliary equation The roots come from solving the quadratic, not from reading off the model.
Check the chosen solution satisfies the model
un+2−un+1+6un=0 The correct general solution satisfies the model for all values of the constants.
Recall how a recurrence generates a sequence
un+1 (or un+2) is built from the earlier term(s) A recurrence relation says how to get the next term from the ones before it, so the whole sequence follows from the starting value(s).
Recall the auxiliary (characteristic) equation
un+2=aun+1+bun ⇒ m2−am−b=0 Trying un=mn in a homogeneous second-order recurrence and dividing by mn gives this quadratic.
Recall the solution for two distinct real roots
un=Aαn+Bβn Each root of the auxiliary equation contributes one geometric term.
Recall the solution for a repeated root
un=(A+Bn)αn A repeated root supplies one solution, so the second carries a factor n.
Recall the solution for complex roots
un=rn(Acosnθ+Bsinnθ) Writing the conjugate roots as r(cosθ±isinθ) turns the solution into a real oscillation.
Recall the fixed point of a first-order model
L=aL+b ⇒ L=1−ab(a=1) A model that settles down must settle to a fixed point of its recurrence.
Recall the condition for a model to settle
∣a∣<1 for the geometric part to die away A growth factor of modulus 1 or more makes the transient persist or explode.
Recall the first-order homogeneous solution
un+1=aun ⇒ un=Aan A constant multiplier each step produces a geometric sequence.
Recall how many starting values are needed
order 1→1 value,order 2→2 values Exactly that many initial conditions are needed to pin the model down.
Recall the standard trial particular solutions
f(n)=c⇒λ; f(n)=cn+d⇒λn+μ; f(n)=ckn⇒λkn The particular solution copies the shape of the forcing term f(n).
Recall the resonance rule
if the trial already solves the homogeneous part, multiply it by n Otherwise the substitution collapses to 0=f(n) and no coefficient works.
Select the general solution
un=A⋅3n+B(−2)n This option satisfies the model for all values of the arbitrary constants.