Electricity-And-Magnetism · Unit 1 · Video 5 · Interactive Practice
Double Integrals: Area, Charge and Volume
IKey Formulas
Formula
Name
What each element carries
A=∫yminymax[∫x1(y)x2(y)dx]dy
Area as an iterated integral
Its own area, dA=dxdy
Q=∬σ(x,y)dxdy
Total charge on a surface
Charge dQ=σdxdy
dA1=rdθdr,dA2=2πrdr
Polar patch and thin ring
Area of a patch, or of a ring when σ=σ(r)
V=∬f(x,y)dxdy
Volume under a surface
Volume of a column of height f
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) of one row; the outer integral stacks the rows into the area.
IIICharge as a Limit of Sums
For σ=kxy with k=1C/m4 on the 3×2 rectangle, the sums ∑σΔA close in on Q=4ka2b2=9C as the cells shrink.
💡 Because σ=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 r
A patch spanning the same angle dθ is longer far from the centre: its arc is rdθ, so dA1=rdθdr.
💡 The ring shortcut dQ=σ(r)2πrdr is valid only when every point of the ring has the same density; for σ(r,θ) the θ integral must be done with σ inside it.
VQuiz Questions
Problem 1 · Charge on a Rectangle
Given: A rectangular plate with corners at (0,0) and (a,b)=(2m,3m) carries surface charge density σ=kxy with k=4C/m4. Find the total charge Q.
✅ Correct!Q=4ka2b2=44⋅4⋅9=36C.
❌ Not quite.∫0axdx=2a2, not a2: each of the two integrations contributes a factor 21.
❌ Not quite. The integrals give Q=9k; you still have to multiply by k=4C/m4, so Q=36C.
❌ Not quite.kab treats k as if it were the density. The density is kxy, which varies over the plate and must be integrated.
❌ Not quite. Do the inner x integral with y held fixed, then the outer y integral; there are only two factors of 21.
Show solution
Inner integral, y fixed along the row:
∫02kxydx=ky222=2ky
Outer integral adds the rows:
Q=∫032kydy=2k232=9k=9⋅4=36C
This agrees with the general result Q=4ka2b2=44⋅22⋅32=36C.
Problem 2 · The Missing Factor r
Given: A disc of radius R=2m carries σ=kr2 with k=3C/m4. Find the total charge Q.
✅ Correct!Q=2πkR4=2π⋅3⋅16=24π≈75.4C.
❌ Not quite. That is ∬kr2dθdr, which omits the factor r in dA1=rdθdr. Without it, dθdr is only a length.
❌ Not quite. That is σ(R)⋅πR2, which uses the rim density everywhere. The density is smaller nearer the centre.
❌ Not quite. The θ integral runs from 0 to 2π and contributes a factor 2π, not 1.
Show solution
Each element carries dQ=σdA1=kr2⋅rdθdr. Do the θ integral first (r fixed):
Given: A region in the xy plane: the row at height y runs from x1(y)=y2 to x2(y)=2y, for 0≤y≤2 (lengths in m). Find the area A of the region.
✅ Correct! The row length is 2y−y2, and ∫02(2y−y2)dy=34m2.
❌ Not quite.∫022ydy=4 measures each row from x=0. The row starts at x1(y)=y2, so subtract it.
❌ Not quite. The inner integral gives x2(y)−x1(y), a difference, not a sum.
❌ Not quite.∫02y2dy=38 is the area to the left of the region. The row length is x2(y)−x1(y).
Show solution
Inner integral: the length of the row at height y,
∫y22ydx=2y−y2
Outer integral adds the rows from ymin=0 to ymax=2:
A=∫02(2y−y2)dy=[y2−3y3]02=4−38=34m2
Check: x2(y)≥x1(y) on [0,2] since 2y−y2=y(2−y)≥0, and the two edges meet at y=0 and y=2.
Problem 4 · When the Ring Shortcut Fails
Given: A disc of radius R=1m carries σ(r,θ)=kr(1+cosθ) with k=3C/m3, so it is denser on the right (θ=0) than on the left. Find the total charge Q.
✅ Correct! The cosθ part integrates to zero around each ring, leaving Q=32πkR3=2πC.
❌ Not quite. That uses the density at θ=0, σ=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 r in the area element rdθdr.
❌ Not quite. Only the cosθ term averages to zero around a ring; the constant 1 in 1+cosθ does not, and σ≥0 everywhere.
Show solution
With no symmetry in θ, do the full integral with σ(r,θ) inside the θ integral:
Q=∫0R[∫02πkr(1+cosθ)rdθ]dr
At fixed r: ∫02π(1+cosθ)dθ=2π+0=2π, so the bracket is 2πkr2.