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Differential Equations First-Order Ordinary Differential Equations Flashcards
59 question-and-answer cards covering First-Order Ordinary Differential Equations as it is examined in Differential Equations. 24 of them are printed below, taken from across the deck — no signup, no paywall on the preview.
24 sample cards from the First-Order Ordinary Differential Equations deck
Sampled from the end of the deck, so these are different cards from the ones shown on the syllabus page.
What does a direction field (slope field) of $y'=f(x,y)$ represent?
At each point $(x,y)$ it draws a short segment with slope $f(x,y)$; solution curves are tangent to these segments everywhere, giving a qualitative picture of solutions without solving.
What is an isocline in a direction field?
An isocline is the curve $f(x,y)=k$ along which all direction-field segments have the same slope $k$; plotting isoclines helps sketch the field efficiently.
Define an autonomous first-order differential equation.
One in which the independent variable does not appear explicitly: $\frac{dy}{dx}=f(y)$. Its slope depends only on $y$.
What are critical points (equilibria) of the autonomous equation $y'=f(y)$?
The constant solutions $y=c$ where $f(c)=0$. They correspond to the zeros of $f$ and appear as horizontal solution lines.
On a phase line, how do you classify a critical point as asymptotically stable, unstable, or semi-stable?
Stable (attractor): arrows point toward it on both sides. Unstable (repeller): arrows point away on both sides. Semi-stable: arrows point toward it on one side and away on the other.
Using the derivative test, when is a critical point $c$ of $y'=f(y)$ asymptotically stable?
If $f(c)=0$ and $f'(c)<0$, then $c$ is asymptotically stable; if $f'(c)>0$ it is unstable. ($f'(c)=0$ is inconclusive.)
Write the Picard iteration formula for the IVP $y'=f(x,y),\ y(x_{0})=y_{0}$.
Equivalent integral equation $y(x)=y_{0}+\int_{x_{0}}^{x} f(t,y(t))\,dt$; iterate $y_{n+1}(x)=y_{0}+\int_{x_{0}}^{x} f\big(t,y_{n}(t)\big)\,dt$ starting from $y_{0}(x)=y_{0}$.
What does the method of successive approximations (Picard iteration) establish theoretically?
Under a Lipschitz condition on $f$ in $y$, the iterates $y_{n}$ converge uniformly to the unique solution of the IVP, providing a constructive proof of existence and uniqueness.
Compute the first two Picard iterates for $y'=y,\ y(0)=1$.
$y_{0}=1$; $y_{1}=1+\int_{0}^{x}1\,dt=1+x$; $y_{2}=1+\int_{0}^{x}(1+t)\,dt=1+x+\frac{x^{2}}{2}$, approaching $e^{x}$.
State the growth/decay model and its solution.
$\frac{dP}{dt}=kP,\ P(0)=P_{0}$ gives $P(t)=P_{0}e^{kt}$. $k>0$ is exponential growth, $k<0$ is decay.
For radioactive decay with half-life $T$, relate the decay constant $k$ to $T$.
From $P(t)=P_{0}e^{kt}$ with $k<0$, $\tfrac12 P_{0}=P_{0}e^{kT}$ gives $k=-\frac{\ln 2}{T}$, i.e. $T=\frac{\ln 2}{|k|}$.
State Newton's law of cooling as a differential equation.
$\frac{dT}{dt}=k\,(T-T_{m})$, where $T$ is the object's temperature, $T_{m}$ the constant ambient temperature, and $k<0$ a constant.
Give the solution of Newton's law of cooling $\frac{dT}{dt}=k(T-T_{m}),\ T(0)=T_{0}$.
$T(t)=T_{m}+(T_{0}-T_{m})e^{kt}$; as $t\to\infty$, $T\to T_{m}$.
Set up the differential equation for a mixing (compartment) problem for the amount of salt $A(t)$.
$\frac{dA}{dt}=R_{in}-R_{out}=(\text{inflow rate}\times\text{inflow conc.})-(\text{outflow rate}\times\frac{A}{V(t)})$, where $V(t)$ is the current volume in the tank.
In a mixing problem, how is the tank volume $V(t)$ determined when inflow and outflow rates differ?
$V(t)=V_{0}+(r_{in}-r_{out})\,t$, where $r_{in},r_{out}$ are the volumetric flow rates; $V$ is constant only when $r_{in}=r_{out}$.
Write the logistic population model differential equation.
$\frac{dP}{dt}=rP\left(1-\frac{P}{K}\right)$, where $r$ is the intrinsic growth rate and $K$ the carrying capacity.
Give the solution of the logistic equation with $P(0)=P_{0}$.
$P(t)=\dfrac{K P_{0}}{P_{0}+(K-P_{0})e^{-rt}}$, so $P(t)\to K$ as $t\to\infty$.
What are the equilibrium solutions of the logistic equation and their stability?
$P=0$ (unstable) and $P=K$ (asymptotically stable). Populations with $0<P_{0}<K$ increase toward $K$; those above $K$ decrease toward $K$.
At what population size does the logistic model predict the fastest growth (maximum $\frac{dP}{dt}$)?
At the inflection point $P=\frac{K}{2}$, where $\frac{d^{2}P}{dt^{2}}=0$ and the growth rate is greatest.
Compare separable, linear, and exact first-order equations by their identifying form.
Separable: $y'=g(x)h(y)$ (variables split). Linear: $y'+P(x)y=Q(x)$ (first power of $y$, use $\mu=e^{\int P}$). Exact: $M\,dx+N\,dy=0$ with $M_{y}=N_{x}$ (potential $F$ exists).
How can you recognize and solve $\frac{dy}{dx}=f(ax+by+c)$?
Substitute $u=ax+by+c$; then $\frac{du}{dx}=a+b\,f(u)$, which is separable in $u$ and $x$.
What is the interval of validity (interval of definition) of a solution to an IVP?
The largest open interval containing $x_{0}$ on which the particular solution is defined, continuous, and satisfies the ODE; it may be smaller than the domain of $f$.
State the superposition-free general solution structure of a linear first-order equation in terms of complementary and particular parts.
$y=y_{c}+y_{p}$, where $y_{c}=ce^{-\int P\,dx}$ solves the homogeneous equation $y'+Py=0$ and $y_{p}$ is any particular solution of $y'+Py=Q$.
For the autonomous logistic-type harvesting model $\frac{dP}{dt}=rP(1-\frac{P}{K})-h$, what determines whether the population can survive?
Whether $f(P)=rP(1-\frac{P}{K})-h$ has real positive critical points; if the constant harvest $h$ exceeds the maximum growth $\frac{rK}{4}$, no equilibrium exists and the population declines to extinction.
What this deck covers
The First-Order Ordinary Differential Equations deck follows the Differential Equations First-Order Ordinary Differential Equations syllabus — 5 chapters and 19 topics — so questions land on material that is genuinely examinable rather than trivia around it. That works out to roughly 11.8 cards per chapter.
Answers are written to be recallable, not just readable — averaging about 137 characters, which is long enough to carry the reasoning and short enough to say out loud.
A deck like this earns its keep on the second and third pass. Read the syllabus first so you know the shape of the subject, then use the cards to find the specific facts that have not stuck.
First-Order Ordinary Differential Equations flashcards FAQ
How many First-Order Ordinary Differential Equations flashcards are in this Differential Equations deck?
59 cards. This page previews 24 of them, sampled evenly across the deck so you can judge the difficulty before installing anything.
Are these Differential Equations flashcards free?
Yes. The preview here is free to read with no signup, and the full 59-card deck is free inside the Examius app.
What do the First-Order Ordinary Differential Equations cards cover?
They follow the Differential Equations First-Order Ordinary Differential Equations syllabus — 5 chapters and 19 topics — so the questions track what is actually examinable.
How should I use these flashcards?
Read the syllabus first so you know the shape of the subject, then drill the deck. Examius schedules each card with spaced repetition, so cards you keep missing come back sooner and ones you know drift further apart.