Electricity-And-Magnetism · Unit 1 · Video 5 · Interactive Practice

Double Integrals: Area, Charge and Volume

IKey Formulas

FormulaNameWhat each element carries
A=∫ymin⁡ymax⁡[∫x1(y)x2(y)dx]dyA = \displaystyle\int_{y_{\min}}^{y_{\max}} \left[\int_{x_1(y)}^{x_2(y)} dx\right] dyArea as an iterated integralIts own area, dA=dx dydA = dx\,dy
Q=∬σ(x,y) dx dyQ = \displaystyle\iint \sigma(x,y)\,dx\,dyTotal charge on a surfaceCharge dQ=σ dx dydQ = \sigma\,dx\,dy
dA1=r dθ dr,dA2=2πr drdA_1 = r\,d\theta\,dr, \quad dA_2 = 2\pi r\,drPolar patch and thin ringArea of a patch, or of a ring when σ=σ(r)\sigma = \sigma(r)
V=∬f(x,y) dx dyV = \displaystyle\iint f(x,y)\,dx\,dyVolume under a surfaceVolume of a column of height ff

Key Insight: The inner integral holds the outer variable fixed and adds one row (or one ring); the outer integral adds the rows. The integrand is whatever one small element carries.

IIArea, One Row at a Time

The inner integral gives the length x2(y)−x1(y)x_2(y) - x_1(y) of one row; the outer integral stacks the rows into the area.

IIICharge as a Limit of Sums

For σ=kxy\sigma = kxy with k=1 C/m4k = 1\ \text{C/m}^4 on the 3×23 \times 2 rectangle, the sums ∑σ ΔA\sum \sigma\,\Delta A close in on Q=ka2b24=9 CQ = \tfrac{k a^2 b^2}{4} = 9\ \text{C} as the cells shrink.

💡 Because σ=kxy\sigma = kxy grows toward the far corner, lower-left samples always undercount and upper-right samples always overcount; the integral is the one value both sums approach.

IVWhy the Polar Patch Carries a Factor rr

A patch spanning the same angle dθd\theta is longer far from the centre: its arc is r dθr\,d\theta, so dA1=r dθ drdA_1 = r\,d\theta\,dr.

💡 The ring shortcut dQ=σ(r) 2πr drdQ = \sigma(r)\,2\pi r\,dr is valid only when every point of the ring has the same density; for σ(r,θ)\sigma(r,\theta) the θ\theta integral must be done with σ\sigma inside it.

VQuiz Questions

Problem 1 · Charge on a Rectangle

Given: A rectangular plate with corners at (0,0)(0,0) and (a,b)=(2 m,3 m)(a, b) = (2\ \text{m}, 3\ \text{m}) carries surface charge density σ=kxy\sigma = kxy with k=4 C/m4k = 4\ \text{C/m}^4. Find the total charge QQ.

✅ Correct! Q=ka2b24=4⋅4⋅94=36 CQ = \tfrac{k a^2 b^2}{4} = \tfrac{4 \cdot 4 \cdot 9}{4} = 36\ \text{C}.
❌ Not quite. ∫0ax dx=a22\int_0^a x\,dx = \tfrac{a^2}{2}, not a2a^2: each of the two integrations contributes a factor 12\tfrac12.
❌ Not quite. The integrals give Q=9kQ = 9k; you still have to multiply by k=4 C/m4k = 4\ \text{C/m}^4, so Q=36 CQ = 36\ \text{C}.
❌ Not quite. k abk\,ab treats kk as if it were the density. The density is kxykxy, which varies over the plate and must be integrated.
❌ Not quite. Do the inner xx integral with yy held fixed, then the outer yy integral; there are only two factors of 12\tfrac12.
Show solution

Inner integral, yy fixed along the row:

∫02kxy dx=ky 222=2ky\int_0^2 kxy\,dx = ky\,\frac{2^2}{2} = 2ky

Outer integral adds the rows:

Q=∫032ky dy=2k 322=9k=9⋅4=36 CQ = \int_0^3 2ky\,dy = 2k\,\frac{3^2}{2} = 9k = 9 \cdot 4 = 36\ \text{C}

This agrees with the general result Q=ka2b24=4⋅22⋅324=36 CQ = \tfrac{k a^2 b^2}{4} = \tfrac{4 \cdot 2^2 \cdot 3^2}{4} = 36\ \text{C}.

Problem 2 · The Missing Factor r

Given: A disc of radius R=2 mR = 2\ \text{m} carries σ=kr2\sigma = kr^2 with k=3 C/m4k = 3\ \text{C/m}^4. Find the total charge QQ.

✅ Correct! Q=πkR42=π⋅3⋅162=24π≈75.4 CQ = \tfrac{\pi k R^4}{2} = \tfrac{\pi \cdot 3 \cdot 16}{2} = 24\pi \approx 75.4\ \text{C}.
❌ Not quite. That is ∬kr2 dθ dr\iint kr^2\,d\theta\,dr, which omits the factor rr in dA1=r dθ drdA_1 = r\,d\theta\,dr. Without it, dθ drd\theta\,dr is only a length.
❌ Not quite. That is σ(R)⋅πR2\sigma(R) \cdot \pi R^2, which uses the rim density everywhere. The density is smaller nearer the centre.
❌ Not quite. The θ\theta integral runs from 00 to 2π2\pi and contributes a factor 2π2\pi, not 11.
Show solution

Each element carries dQ=σ dA1=kr2⋅r dθ drdQ = \sigma\,dA_1 = kr^2 \cdot r\,d\theta\,dr. Do the θ\theta integral first (rr fixed):

Q=∫0R[∫02πkr3 dθ]dr=∫0R2πkr3 dr=2πkR44=πkR42Q = \int_0^R \left[\int_0^{2\pi} kr^3\,d\theta\right] dr = \int_0^R 2\pi k r^3\,dr = \frac{2\pi k R^4}{4} = \frac{\pi k R^4}{2} Q=π⋅3⋅242=24π≈75.4 CQ = \frac{\pi \cdot 3 \cdot 2^4}{2} = 24\pi \approx 75.4\ \text{C}

Problem 3 · Rows with Moving Ends

Given: A region in the xyxy plane: the row at height yy runs from x1(y)=y2x_1(y) = y^2 to x2(y)=2yx_2(y) = 2y, for 0≤y≤20 \le y \le 2 (lengths in m). Find the area AA of the region.

✅ Correct! The row length is 2y−y22y - y^2, and ∫02(2y−y2) dy=43 m2\int_0^2 (2y - y^2)\,dy = \tfrac43\ \text{m}^2.
❌ Not quite. ∫022y dy=4\int_0^2 2y\,dy = 4 measures each row from x=0x = 0. The row starts at x1(y)=y2x_1(y) = y^2, so subtract it.
❌ Not quite. The inner integral gives x2(y)−x1(y)x_2(y) - x_1(y), a difference, not a sum.
❌ Not quite. ∫02y2 dy=83\int_0^2 y^2\,dy = \tfrac83 is the area to the left of the region. The row length is x2(y)−x1(y)x_2(y) - x_1(y).
Show solution

Inner integral: the length of the row at height yy,

∫y22ydx=2y−y2\int_{y^2}^{2y} dx = 2y - y^2

Outer integral adds the rows from ymin⁡=0y_{\min} = 0 to ymax⁡=2y_{\max} = 2:

A=∫02(2y−y2) dy=[y2−y33]02=4−83=43 m2A = \int_0^2 (2y - y^2)\,dy = \left[y^2 - \frac{y^3}{3}\right]_0^2 = 4 - \frac{8}{3} = \frac{4}{3}\ \text{m}^2

Check: x2(y)≥x1(y)x_2(y) \ge x_1(y) on [0,2][0, 2] since 2y−y2=y(2−y)≥02y - y^2 = y(2 - y) \ge 0, and the two edges meet at y=0y = 0 and y=2y = 2.

Problem 4 · When the Ring Shortcut Fails

Given: A disc of radius R=1 mR = 1\ \text{m} carries σ(r,θ)=k r (1+cos⁡θ)\sigma(r, \theta) = k\,r\,(1 + \cos\theta) with k=3 C/m3k = 3\ \text{C/m}^3, so it is denser on the right (θ=0\theta = 0) than on the left. Find the total charge QQ.

✅ Correct! The cos⁡θ\cos\theta part integrates to zero around each ring, leaving Q=2πkR33=2π CQ = \tfrac{2\pi k R^3}{3} = 2\pi\ \text{C}.
❌ Not quite. That uses the density at θ=0\theta = 0, σ=2kr\sigma = 2kr, for the whole ring. Points on one ring carry different densities here, so the ring shortcut does not apply.
❌ Not quite. That omits the factor rr in the area element r dθ drr\,d\theta\,dr.
❌ Not quite. Only the cos⁡θ\cos\theta term averages to zero around a ring; the constant 11 in 1+cos⁡θ1 + \cos\theta does not, and σ≥0\sigma \ge 0 everywhere.
Show solution

With no symmetry in θ\theta, do the full integral with σ(r,θ)\sigma(r,\theta) inside the θ\theta integral:

Q=∫0R[∫02πk r (1+cos⁡θ) r dθ]drQ = \int_0^R \left[\int_0^{2\pi} k\,r\,(1 + \cos\theta)\,r\,d\theta\right] dr

At fixed rr: ∫02π(1+cos⁡θ) dθ=2π+0=2π\int_0^{2\pi} (1 + \cos\theta)\,d\theta = 2\pi + 0 = 2\pi, so the bracket is 2πkr22\pi k r^2.

Q=∫0R2πkr2 dr=2πkR33=2π⋅3⋅13=2π≈6.28 CQ = \int_0^R 2\pi k r^2\,dr = \frac{2\pi k R^3}{3} = \frac{2\pi \cdot 3 \cdot 1}{3} = 2\pi \approx 6.28\ \text{C}

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