This page is the drill ground for Changing order of integration . The parent taught you the 5-step recipe; here we run it against every kind of region the topic can hand you — and we do not skip a single case. Before any example, we lay out a matrix of scenarios so you can see the whole battlefield.
Intuition What "every scenario" means here
A change-of-order problem is fully described by three questions :
What curves bound the region (line? parabola? circle? two curves crossing)?
Does the region need splitting in one orientation (multiple strips) but not the other?
Is there a degenerate/limiting feature (a zero-width point, an unbounded piece, a strip that exits onto a different curve halfway up)?
If you can handle each row of the table below, no exam version can surprise you.
Cell
Region shape
The twist you must survive
Example
C1
Triangle (line + axes)
inner has no elementary antiderivative — reorder to save it
Ex 1
C2
Lens (two curves cross: line vs parabola)
must re-solve both boundaries for the new variable, pick correct branch
Ex 2
C3
Region needing a split one way
one orientation = 2 integrals, other = 1 clean integral
Ex 3
C4
Strip that exits onto different curves at different heights
the exit boundary switches — you MUST split
Ex 4
C5
Degenerate corner / zero-width tip
boundaries meet at a point; check the limit is fine, not undefined
Ex 5
C6
Circle / disk piece
reorder AND recognise polar is even better
Ex 6
C7
Word problem (real-world total)
translate physical region into limits, then reorder to compute
Ex 7
C8
Exam twist: unknown/general f , symbolic answer
reorder without ever evaluating f
Ex 8
Every cell C1–C8 is hit below. Numeric answers are all machine-checked in the verify block.
Evaluate I = ∫ 0 1 ∫ x 1 e y 2 d y d x .
Forecast: Guess before reading — will the answer contain e ? Will reordering make the y -integral doable? (Hold that thought.)
Step 1 — Read the limits. Outer 0 ≤ x ≤ 1 ; inner x ≤ y ≤ 1 .
Why this step? The limits ARE the region. Reading them out loud gives us the boundary curves: the bottom of each vertical strip rides on the line y = x , the top on the line y = 1 .
Step 2 — Sketch (look at Figure s01). Above y = x , below y = 1 , right of x = 0 : a triangle with corners ( 0 , 0 ) , ( 0 , 1 ) , ( 1 , 1 ) .
Why this step? ∫ e y 2 d y has no elementary antiderivative , so the given order is a dead end. The sketch tells us the alternative order.
Step 3 — New outer variable y . From the picture the whole region spans 0 ≤ y ≤ 1 .
Why this step? The lowest tile sits at y = 0 (the corner), the highest at y = 1 (the top edge). Outer limits must be pure numbers .
Step 4 — New inner variable x . Fix a height y and slide a horizontal strip (red in the figure). It enters at the left wall x = 0 and exits at the slanted boundary y = x , i.e. x = y . So 0 ≤ x ≤ y .
Why this step? We must re-express the boundary y = x as a formula for the new inner variable: solve y = x for x ⇒ x = y .
Step 5 — Rewrite & evaluate.
I = ∫ 0 1 ∫ 0 y e y 2 d x d y = ∫ 0 1 e y 2 [ x ] 0 y d y = ∫ 0 1 y e y 2 d y .
Substitute u = y 2 , d u = 2 y d y : I = 2 1 ∫ 0 1 e u d u = 2 1 ( e − 1 ) .
Verify: Numerically 2 1 ( e − 1 ) ≈ 0.8591 . Sanity: the integrand e y 2 ≥ 1 over a triangle of area 2 1 , so I ≥ 2 1 — consistent. ✓
Evaluate J = ∫ 0 1 ∫ x 2 x ( x + y ) d y d x .
Forecast: The region is the sliver between y = x and y = x 2 . Guess: after reordering, will the left edge be the line or the parabola?
Step 1 — Read. 0 ≤ x ≤ 1 , x 2 ≤ y ≤ x .
Why this step? Bottom of each vertical strip rides the parabola y = x 2 ; top rides the line y = x . They coincide at x = 0 and x = 1 .
Step 2 — Sketch (Figure s02). A lens-shaped region between line (upper) and parabola (lower), corners ( 0 , 0 ) , ( 1 , 1 ) .
Why this step? We need to know, for a fixed height y , which curve is on the left and which on the right .
Step 3 — New outer y : 0 ≤ y ≤ 1 .
Why this step? Lowest and highest points of the lens are the two corners.
Step 4 — New inner x . For fixed y ∈ ( 0 , 1 ) , solve each boundary for x :
line y = x ⇒ x = y ,
parabola y = x 2 ⇒ x = y (positive branch — the region lives in the first quadrant).
Since 0 < y < 1 gives y < y , the strip runs y ≤ x ≤ y .
Why this step? We MUST re-solve both boundaries and pick the branch that lies in R . Test y = 4 1 : strip [ 0.25 , 0.5 ] — both inside the lens. ✓
Step 5 — Evaluate both ways (they must match).
Original order:
J = ∫ 0 1 ∫ x 2 x ( x + y ) d y d x = ∫ 0 1 [ x y + 2 y 2 ] x 2 x d x = ∫ 0 1 ( 2 3 x 2 − x 3 − 2 x 4 ) d x .
= 2 1 − 4 1 − 10 1 = 20 3 .
Reordered check: J = ∫ 0 1 ∫ y y ( x + y ) d x d y = 20 3 too.
Verify: J = 20 3 = 0.15 , both orders agree. ✓
Reverse the order and evaluate S = ∫ 0 2 ∫ 0 x y d y d x + ∫ 2 4 ∫ 0 4 − x y d y d x .
This is the total over the triangle with vertices ( 0 , 0 ) , ( 4 , 0 ) , ( 2 , 2 ) , written as two vertical-strip integrals (it needed splitting at x = 2 where the top edge changes from y = x to y = 4 − x ).
Forecast: Guess: can horizontal strips describe this triangle in ONE integral (no split)?
Step 1 — Read. Left piece: 0 ≤ x ≤ 2 , 0 ≤ y ≤ x . Right piece: 2 ≤ x ≤ 4 , 0 ≤ y ≤ 4 − x .
Why this step? Two pieces because the top boundary of a vertical strip is y = x for x < 2 but y = 4 − x for x > 2 — the exit curve switches at the apex.
Step 2 — Sketch (Figure s03). A triangle: base on the x -axis from 0 to 4 , apex at ( 2 , 2 ) .
Why this step? The picture shows that a horizontal strip at height y enters on the left edge y = x ⇒ x = y and exits on the right edge y = 4 − x ⇒ x = 4 − y , for ALL y — no split needed.
Step 3 — New outer y : 0 ≤ y ≤ 2 .
Why this step? Apex height is 2 , base at 0 .
Step 4 — New inner x : y ≤ x ≤ 4 − y .
Why this step? Both edges solved for x ; one single description works.
Step 5 — Evaluate the single integral.
S = ∫ 0 2 ∫ y 4 − y y d x d y = ∫ 0 2 y [ ( 4 − y ) − y ] d y = ∫ 0 2 y ( 4 − 2 y ) d y = ∫ 0 2 ( 4 y − 2 y 2 ) d y .
= [ 2 y 2 − 3 2 y 3 ] 0 2 = 8 − 3 16 = 3 8 .
Verify: S = 3 8 ≈ 2.667 . Cross-check by summing the two original pieces: ∫ 0 2 2 x 2 d x + ∫ 2 4 2 ( 4 − x ) 2 d x = 3 4 + 3 4 = 3 8 . ✓ (Reordering turned 2 integrals into 1.)
Reverse the order in T = ∫ 0 2 ∫ x 2 2 x f ( x , y ) d y d x (region between y = x 2 and y = 2 x ).
Forecast: The curves cross at ( 0 , 0 ) and ( 2 , 4 ) . Guess: when we use horizontal strips, does one exit curve serve the whole height, or does it switch?
Step 1 — Read. 0 ≤ x ≤ 2 , x 2 ≤ y ≤ 2 x . On [ 0 , 2 ] , x 2 ≤ 2 x , so the parabola is below the line.
Why this step? Establishes the region: below the line y = 2 x , above the parabola y = x 2 .
Step 2 — Sketch (Figure s04). A curved sliver from ( 0 , 0 ) to ( 2 , 4 ) .
Why this step? We check where a horizontal strip enters/exits. Solve for x : line y = 2 x ⇒ x = y /2 ; parabola y = x 2 ⇒ x = y (positive branch). For 0 < y < 4 , y /2 < y — the strip runs y /2 ≤ x ≤ y , and this holds for the WHOLE range 0 ≤ y ≤ 4 .
Step 3 — New outer y : 0 ≤ y ≤ 4 (apex at ( 2 , 4 ) ).
Step 4 — New inner x : 2 y ≤ x ≤ y .
Why this step? Both boundaries re-solved for x ; correct branch of ⋅ chosen (region in first quadrant). Test y = 1 : strip [ 0.5 , 1 ] ; check the midpoint ( 0.7 , 1 ) satisfies 0.49 ≤ 1 ≤ 1.4 ✓.
Step 5 — Result.
T = ∫ 0 4 ∫ y /2 y f ( x , y ) d x d y .
To make it concrete, take f = 1 (area). Original: ∫ 0 2 ( 2 x − x 2 ) d x = 4 − 3 8 = 3 4 . Reordered: ∫ 0 4 ( y − 2 y ) d y = 3 2 ⋅ 8 − 4 1 ⋅ 16 = 3 16 − 4 = 3 4 . ✓
Verify: area = 3 4 both orders. ✓ (Here the exit curve did NOT switch — contrast Ex 3 where it did. Reading the picture is what tells you which.)
Reverse the order in U = ∫ 0 1 ∫ 0 1 − x 2 x d y d x — a quarter disk. Watch the degenerate corners where the strip width shrinks to zero.
Forecast: At x = 1 the top boundary 1 − x 2 = 0 : the vertical strip has zero height. Guess: does that cause any trouble in either order?
Step 1 — Read. 0 ≤ x ≤ 1 , 0 ≤ y ≤ 1 − x 2 : the quarter of the unit circle in the first quadrant.
Why this step? y = 1 − x 2 is the upper arc x 2 + y 2 = 1 .
Step 2 — Sketch (Figure s05). Quarter disk, corners ( 0 , 0 ) , ( 1 , 0 ) , ( 0 , 1 ) .
Why this step? At x → 1 the strip height → 0 (a degenerate tip at ( 1 , 0 ) ). Integrands stay finite, so the integral is a proper (non-improper) integral — no blow-up.
Step 3 — New outer y : 0 ≤ y ≤ 1 .
Step 4 — New inner x : solve arc y = 1 − x 2 ⇒ x = 1 − y 2 (positive branch). So 0 ≤ x ≤ 1 − y 2 .
Why this step? Horizontal strip enters at wall x = 0 , exits at arc x = 1 − y 2 . At y → 1 this width → 0 — the SAME degenerate tip, now at the top. The formula is still finite there, confirming no problem.
Step 5 — Evaluate.
U = ∫ 0 1 ∫ 0 1 − y 2 x d x d y = ∫ 0 1 2 1 ( 1 − y 2 ) d y = 2 1 [ y − 3 y 3 ] 0 1 = 2 1 ⋅ 3 2 = 3 1 .
Verify: Original order: ∫ 0 1 x 1 − x 2 d x = [ − 3 1 ( 1 − x 2 ) 3/2 ] 0 1 = 3 1 . Both give 3 1 ; the degenerate tip contributed no defect. ✓
Consider V = ∫ 0 1 ∫ 0 1 − x 2 ( x 2 + y 2 ) d y d x over the same quarter disk. Reorder — then note Polar Coordinates in Double Integrals is even cleaner.
Forecast: Guess whether the Cartesian reorder is pleasant, or whether you'd rather switch to r , θ .
Step 1 — Read & sketch. Same quarter disk as Ex 5 (reuse Figure s05).
Why this step? Region identical; only the integrand changed to x 2 + y 2 .
Step 2 — Reorder (Cartesian). By the same solving as Ex 5:
V = ∫ 0 1 ∫ 0 1 − y 2 ( x 2 + y 2 ) d x d y .
Why this step? Shows the reorder is valid, but the inner integral ∫ ( x 2 + y 2 ) d x = 3 x 3 + y 2 x evaluated at x = 1 − y 2 is messy.
Step 3 — Switch to polar. On the quarter disk: x 2 + y 2 = r 2 , d A = r d r d θ , with 0 ≤ r ≤ 1 , 0 ≤ θ ≤ 2 π .
Why this step? Why polar and not more Cartesian gymnastics? Because the region is a circular arc and the integrand depends only on r — polar makes the limits constants and separates the integral. This is exactly what Change of Variables (Jacobian) formalises (the Jacobian gives the r factor).
Step 4 — Evaluate.
V = ∫ 0 π /2 ∫ 0 1 r 2 ⋅ r d r d θ = ∫ 0 π /2 [ 4 r 4 ] 0 1 d θ = 4 1 ⋅ 2 π = 8 π .
Verify: V = 8 π ≈ 0.3927 . (Cartesian reorder gives the same after grinding.) ✓
A triangular metal plate has vertices ( 0 , 0 ) , ( 2 , 0 ) , ( 0 , 2 ) (units: cm). Its surface density is ρ ( x , y ) = e y 2 g/cm². The mass is M = ∬ R e y 2 d A . Set it up in the convenient order and compute.
Forecast: Guess: which variable must be the outer one so the inner integral is doable?
Step 1 — Translate the plate into a region. The triangle is bounded by x = 0 , y = 0 , and the line through ( 2 , 0 ) , ( 0 , 2 ) : x + y = 2 , i.e. 0 ≤ x ≤ 2 − y . So R : 0 ≤ y ≤ 2 , 0 ≤ x ≤ 2 − y .
Why this step? A word problem is just a region + integrand in disguise; we must extract both.
Step 2 — Sketch (Figure s06).
Why this step? Confirms the hypotenuse x + y = 2 and which order makes e y 2 integrable.
Step 3 — Choose y as OUTER. If y were inner we'd face ∫ e y 2 d y — impossible. With y outer, the inner x -integral treats e y 2 as a constant.
Why this step? Same lesson as Ex 1: put the "impossible" variable on the OUTSIDE.
Step 4 — Inner limits. For fixed y , x runs 0 to 2 − y .
Why this step? Left wall x = 0 , right boundary the hypotenuse x = 2 − y .
Step 5 — Evaluate.
M = ∫ 0 2 ∫ 0 2 − y e y 2 d x d y = ∫ 0 2 ( 2 − y ) e y 2 d y .
Split: ∫ 0 2 2 e y 2 d y − ∫ 0 2 y e y 2 d y . The second is elementary: 2 1 ( e 4 − 1 ) . The first is a genuine non-elementary integral (see Improper and Non-elementary Integrals ); write it as 2 ∫ 0 2 e y 2 d y , a value ≈ 2 ( 16.4526 ) = 32.905 .
M ≈ 32.905 − 2 1 ( e 4 − 1 ) = 32.905 − 26.799 = 6.106 g .
Why this step? Even here, reordering isolated the elementary chunk; the remaining term is honestly non-elementary and must be evaluated numerically.
Verify: M ≈ 6.11 g. Sanity by units: g/cm² × cm² = g ✓. Sanity by bound: area = 2 cm², density between 1 and e 4 ≈ 54.6 , and mass 6.1 lies in [ 2 , 109 ] ✓.
Reverse the order of integration, without evaluating , for
W = ∫ 0 2 ∫ 0 y /2 f ( x , y ) d x d y + ∫ 2 4 ∫ 0 2 − y /2 + ? …
— actually the clean twist: reverse W = ∫ 0 1 ∫ − y y f ( x , y ) d x d y . This region is symmetric across x = 0 , so it spans quadrants left and right of the y -axis.
Forecast: Both signs of x appear. Guess: after reordering, does the region split at x = 0 , and what are the two branches?
Step 1 — Read. 0 ≤ y ≤ 1 , − y ≤ x ≤ y : the region under the parabola y = x 2 opening upward, capped at y = 1 , symmetric about the y -axis.
Why this step? x = ± y are the two branches of y = x 2 ; both signs of x occur, so we must handle negative-x and positive-x tiles.
Step 2 — Sketch (Figure s07).
Why this step? Shows the region is a parabolic cap over − 1 ≤ x ≤ 1 , bounded below by y = x 2 and above by y = 1 .
Step 3 — New outer x : overall − 1 ≤ x ≤ 1 .
Why this step? Widest tiles are at y = 1 where x = ± 1 . Note the outer variable now takes negative values — a case the naive "min=0" habit would miss.
Step 4 — New inner y : for a fixed x , vertical strip enters at the parabola y = x 2 and exits at y = 1 . So x 2 ≤ y ≤ 1 . This single description covers BOTH signs of x because x 2 is even — no split needed .
Why this step? Re-solving the boundary x = ± y for y gives the single curve y = x 2 , which merges the two branches.
Step 5 — Result.
W = ∫ − 1 1 ∫ x 2 1 f ( x , y ) d y d x .
Why this step? Fully symbolic; valid for any integrable f by Fubini's Theorem over this general region .
Verify (with a concrete f = 1 , i.e. area): original ∫ 0 1 2 y d y = 2 ⋅ 3 2 = 3 4 ; reordered ∫ − 1 1 ( 1 − x 2 ) d x = 2 − 3 2 = 3 4 . Both = 3 4 , confirming the reorder (and that negative x was correctly included). ✓
Recall Which cell does each trap live in?
"Left the outer limit as a curve" happens most in which cell type? ::: The word/general ones (C7, C8) — always reduce the OUTER limits to constants.
When does reordering turn 2 integrals into 1? ::: When the exit curve switches in one orientation but not the other (C3).
When is the negative branch of a square root the correct one? ::: When the region lies left of the y -axis (C8) — pick the branch that lands in R .
Mnemonic The matrix in one breath
"Triangle, Lens, Split, Switch, Tip, Disk, Word, Symbol" — C1→C8. If your problem doesn't feel like one of these eight, you've mis-sketched.