Picture a single number that changes as time passes: the temperature of a cooling cup of coffee, the height of a bouncing-then-settling swing, the charge left on a battery.
Look at the blue curve above: at each moment t (a spot on the bottom axis) the curve is at some height. That height is the single number y(t). The entire blue curve is the function; one dot on it is one value y(t). Reading the curve left-to-right is watching the system evolve.
Why the topic needs this: everything in stiff equations is about how such a curve decays toward zero and how well a computer can trace it.
A computer cannot store the whole curve; it can only know the value now and a rule for how fast it is changing. That rate of change is the derivative.
The green line is the tangent — the straight line that touches the curve and matches its slope at that one spot. Its steepness is the number y′.
Why "derivative" and not some other tool? Because a differential equation is a machine that hands you the slope at every point and asks you to reconstruct the curve. Slope is exactly the language it speaks.
Read it aloud: "the rate of change of y equals some formula involving the current time and the current y."
But a slope-rule alone is not enough. Knowing the slope everywhere tells you the shape of the curve, not where it starts. Infinitely many parallel curves have the same slope-rule; we must pin down one.
Why the topic needs this: the whole subject studies one master IVP, y′=λy with y(0)=y0, because it is the simplest decay-rule and every method's behaviour shows up cleanly in it.
But eλt is not the only solution of y′=λy — any constant multiple works too, because scaling a curve scales its slope by the same factor. The starting value y0 from Section 3 fixes which multiple:
Two decaying curves: λ=−1 (gentle, yellow) and λ=−100 (a cliff, red). Both head to zero, but the red one is essentially gone almost instantly. A stiff problem contains both shapes at once — and that clash of speeds is the whole difficulty.
Sometimes λ is a complex number (it has a "real part" and an "imaginary part") because oscillations hide inside it. You do not need complex analysis here — only one word.
Why the topic needs it: real systems (springs, circuits) decay and oscillate. Writing Reλ<0 lets one clean inequality cover them all.
A computer cannot handle a smooth continuum. It jumps forward in fixed hops.
The smooth blue curve is the truth; the yellow dots are the computer's samples y0,y1,y2,… spaced h apart. The very first dot y0 is handed to us by the initial condition; numerical methods are recipes for getting the next dot from the current one.
Here is where "slope" meets "hops". A slope is rise over run. Over one hop, the run is h and the rise is the change in y.
This is the bridge from the exact world (Section 2) to the computable world (Section 6). Which dot's slope this rise-over-run represents — the old dot tn or the new dot tn+1 — is the single choice that splits forward Euler (explicit) from backward Euler (implicit). That choice is the heart of the parent topic; you now have every symbol to understand it.
Why the topic needs it: a method is stable when, step after step, it shrinks the value toward zero rather than blowing it up. "Does it shrink?" is exactly "is the multiplier's magnitude below 1?" — written ∣multiplier∣<1. Sign doesn't matter (a value could flip sign each step and still shrink); only size does. That is why absolute value, not the plain number, rules stability.
Each foundation feeds the next: time and value make a curve, the curve has a slope, the slope-rule plus a starting value y0 is an IVP, the IVP's answer is a scaled exponential, mixing fast and slow exponentials makes stiffness, and the finite-difference slope plus the size-test decide whether a method survives.