Intuition The one core idea
An RL circuit — short for a R esistor and an indL uctor wired one-after-another (in series) with a battery — has an inductor that stores energy in a magnetic field, and that stored energy gives the electric current a kind of inertia : the current cannot start or stop instantly, it can only ease in and ease out. Everything in RL transient behavior is just this one idea written as math: how fast the current eases, and the single number τ = L / R that sets the pace.
Definition What "RL" means
Throughout this topic, RL is shorthand for a resistor–inductor series circuit : a battery, a resistor R , and an inductor L all connected in a single loop. "R" is the resistor, "L" is the inductor (the standard symbol for inductance). That is the only circuit we study here.
Before you can read the parent note RL Transient Behavior , you must be able to read every letter and squiggle it uses without pausing. This page builds each one from nothing, in an order where each piece rests on the one before it.
i ( t )
Current is how much electric charge passes a point in a wire every second . The symbol is i (lower-case, because it can change over time) and its unit is the ampere (A). We write i ( t ) to remind ourselves it is a function of time — its value depends on when you look.
Picture a pipe with water flowing. The current is not the water — it is the rate of water passing a marked line each second. In this whole topic, i is the star: it starts somewhere, changes, and settles.
Why the topic needs it: the entire RL story is the shape of the curve i ( t ) — how the flow builds up or dies away after you flip a switch.
Voltage is the electrical push that drives current, measured in volts (V). We use two styles:
Capital V for a fixed push that does not change (the battery/source).
Lower-case v (like v R , v L ) for a push that varies over time across one component.
Voltage is the pressure ; current is the flow it causes . A tall water tank (big voltage) pushes harder, so more water flows (more current) — unless something resists.
Why the topic needs it: the source V is the cause; the current i is the effect. We track how the total push V splits between the resistor and the inductor.
Before we add voltages up, we must agree on which direction counts as positive . Otherwise a minus sign appears out of nowhere and the reader is lost.
Definition Passive sign convention
Pick one direction around the loop as the positive direction of current i (say, clockwise, the way the battery pushes). For each passive component (resistor, inductor), the arrow of its voltage points against the current flow — the current enters the + terminal and leaves the − terminal . This means a positive current produces a positive drop v R = i R , and the battery's push V points with the current.
Intuition What the signs look like
Imagine walking around the loop in the current's direction. You gain height at the battery (a rise, + V ) and lose height across each passive component (a drop, − v R , − v L ). Adding all rises and drops must return you to the same height — that is the loop rule of the next sections.
Common mistake Edge case: what if current is
falling or negative ?
During discharge the current is decreasing, so d i / d t < 0 . Plug that into v L = L d i / d t and v L comes out negative — the inductor's voltage reverses and now acts like a little battery, pushing current to keep flowing. The formulas still hold with no special cases: just let the signs be what they are. A negative v L simply means the inductor is giving back stored energy instead of absorbing it.
Why the topic needs it: without a fixed sign convention, V = i R + L d i / d t is ambiguous. With it, the same equation covers rising, falling, and negative currents automatically.
R
Resistance measures how much a component fights the flow of current, in ohms (Ω ). More resistance → less current for the same push.
Picture a narrow section of pipe: it resists flow, and the "pressure drop" across it grows if either more water flows (i ) or the pipe is narrower (bigger R ).
Why the topic needs it: the resistor is one of the two components in the loop, and v R = i R is one of the two voltage terms in the loop equation.
L
An inductor is a coil of wire. When current flows through it, it stores energy in a magnetic field wrapped around the coil. Inductance L (unit: henry , H) measures how strongly it stores that field — i.e. how much it resists a change in current.
A heavy flywheel resists changes in its spin: hard to speed up, hard to stop. An inductor does the same to current. The stored magnetic energy is like the flywheel's spinning energy — it has to be built up or drained, and that takes time.
Why the topic needs it: this "inertia" is the entire reason the current cannot jump instantly. Without L , there would be no transient at all — just Ohm's law. See Inductor Fundamentals for where this comes from.
This is the symbol that scares people. Let us build it from zero.
Definition The derivative
d t d i
d t d i means "how fast i is changing right now ." It is the slope of the current curve at one instant: rise in current divided by the tiny time it took.
d i = a tiny change in current.
d t = the tiny slice of time that change happened in.
The ratio = change-per-second = the steepness of the i ( t ) graph.
Intuition Slope is a picture, not algebra
Look back at figure s01. Where the current curve is steep , d i / d t is large (current changing fast). Where the curve flattens out , d i / d t → 0 (current barely changing). Steady state = flat line = zero slope. When current falls , the slope is negative — the curve tilts downward.
Why this tool and not another? We need a quantity that captures change over time . Plain subtraction (i 2 − i 1 ) needs two separate moments; the derivative gives the rate at a single instant , which is exactly what the inductor reacts to. That is why the derivative — and not, say, an average — is the right tool here.
Read it in plain words: the harder you try to change the current, the harder the inductor pushes back.
Current steady (d i / d t = 0 ) → v L = 0 → the inductor is just plain wire (a "short").
Try to change current instantly (jump in zero time) → d i / d t = ∞ → v L = ∞ . Impossible! So current is forced to be continuous : i ( 0 + ) = i ( 0 − ) .
Current decreasing (d i / d t < 0 ) → v L < 0 → the inductor's voltage flips sign and it feeds current back (the discharge case from §3).
Why the topic needs it: this single law, combined with the loop equation, produces the whole exponential curve.
Walk once around any closed loop of a circuit, adding up every voltage push and drop. The total must be zero — pushes from sources equal drops across components. Using the sign convention from §3, for our series loop:
V = v R + v L = i R + L d t d i
Intuition Why it must be true
Voltage is energy per charge. If you walk a full loop and return to the start, you are back where you began — no net energy gained or lost per charge. So the ups and downs cancel exactly.
Why the topic needs it: this is the starting line of the whole derivation. See Kirchhoff's Voltage Law .
The derivation in the parent note uses two symbols you should recognize, even if you never solve one by hand.
ln
ln is the "undo" button for the exponential . Since e x takes a number and grows it, ln takes the result and gives you back x . In symbols: ln ( e x ) = x . It is the tool that lets us isolate the time t once it is trapped inside an exponential.
∫
The symbol ∫ (a stretched "S" for "sum") means add up infinitely many tiny pieces . If d i / d t is the rate of change over each tiny slice, then ∫ stitches all those slices back into the total change. It is the opposite operation to the derivative d i / d t .
Intuition Why these two, here?
The loop equation mixes i and its rate d i / d t . To untangle them we integrate (add up the tiny changes) — and that integration naturally produces a ln , which we then undo with e to get a clean formula for i ( t ) . See First-Order Differential Equations for the full mechanics; here you only need to know what the two symbols mean .
Definition Euler's number
e
e ≈ 2.718 is a special constant. The function e − t / τ is the natural shape of anything that fades toward zero at a rate proportional to how much is left — like a hot cup cooling, or here, a settling current.
Intuition Why exponentials show up everywhere
When the speed of change is proportional to the amount remaining , you get an exponential — no other shape fits. In our circuit, L d i / d t = V − i R : the rate of change (d i / d t ) is proportional to how far the current still has to go. That proportionality is the fingerprint of the exponential.
Key facts about e − t / τ you will use:
At t = 0 : e 0 = 1 (full value).
As t → ∞ : e − ∞ = 0 (faded away).
At t = τ : e − 1 ≈ 0.368 (dropped to 36.8% of its start).
Why the topic needs it: the settling current is a pure exponential — that is the shape of every RL transient.
Definition Initial current
I 0
I 0 (capital I , subscript zero, read "eye-nought") is the current already flowing at the moment t = 0 , the instant the switch flips. The subscript 0 literally marks "time zero." During a discharge , the source is removed but the inductor's inertia keeps this current flowing, and it fades away from I 0 down to zero.
Intuition Picture the starting line
Think of I 0 as the speed of the rolling shopping cart at the exact moment you stop pushing. It does not stop dead — it coasts from that starting speed and slows down. I 0 is that starting speed for the current.
Why the topic needs it: the discharge formula begins at I 0 ; without naming it we could not write the decay curve.
τ
τ (the Greek letter "tau") is a single number, in seconds, that sets how fast the transient happens. For an RL circuit:
τ = R L
Big L (more inertia) → bigger τ → slower. Big R (drains energy faster) → smaller τ → faster.
Common mistake Units check: is
L / R really seconds?
ohm henry = V / A V⋅s / A = s ✓
If you had written τ = R L or R / L , the units would come out wrong — a quick sanity check. See Time Constant .
Why the topic needs it: τ is the one number that summarizes the whole curve's speed. After about 5 τ the transient is over (see Steady-State Analysis ).
Now every symbol below is defined. These are the two results the parent note derives; here they simply show you the destination.
Every letter here — i , V , R , L , τ , e , I 0 — was built in the sections above. You are ready.
Self-test: can you say each of these out loud before reading the parent note?
What does "RL circuit" stand for? A resistor (R ) and inductor (L ) wired in series with a source.
What does i ( t ) mean, in plain words? How much charge passes a point per second, as a function of time (unit: ampere).
What is the difference between V and v L ? V is a fixed source push; v L is the time-varying voltage across the inductor.
State the passive sign convention in one line. Pick a positive current direction; passive components drop voltage against that direction, so v R = i R is positive for positive i .
What happens to v L when the current is falling (d i / d t < 0 )? v L goes negative — the inductor reverses and feeds current back.
State Ohm's law for the resistor's voltage. v R = i R .
In one sentence, what does an inductor store and why does that matter? It stores energy in a magnetic field, giving current inertia so it cannot change instantly.
What does d t d i measure, and what does it look like on a graph? The rate of change of current — the slope (steepness) of the i ( t ) curve at an instant.
Write the inductor's voltage law. v L = L d t d i .
What does ln do, and what does ∫ do? ln undoes an exponential; ∫ adds up infinitely many tiny pieces (opposite of the derivative).
Why can't current jump instantly in an inductor? An instant jump means d i / d t = ∞ , which needs infinite voltage — impossible, so i is continuous.
State KVL for the series RL loop. V = i R + L d t d i .
What is I 0 ? The current already flowing at t = 0 — the starting value for a discharge.
What is e − t / τ at t = 0 and at t = τ ? 1 at t = 0 ; about 0.368 (36.8%) at t = τ .
Write the time constant and confirm its units. τ = L / R ; henry/ohm = seconds.