DOC PREVIEW
HARVARD MATH 21A - 2D INTEGRATION

This preview shows page 1 out of 2 pages.

Save
View full document
View full document
Premium Document
Do you want full access? Go Premium and unlock all 2 pages.
Access to all documents
Download any document
Ad free experience
Premium Document
Do you want full access? Go Premium and unlock all 2 pages.
Access to all documents
Download any document
Ad free experience

Unformatted text preview:

11/12/2002, 2D INTEGRATION Math 21a, O. KnillHomework: Section 12.2: 2, 14, 20 12.3 30, 401D INTEGRATION IN 100 WORDS. If f (x) is a continuous function of one variable, thenR10f(x) dx canbe defined as a limit of the Riemann sum fn(x) =1nPnk=1f(xk) for n → ∞ with xk= k/n. The in-tegral is the average of f on the interval [a, b]. It can be interpreted as an signed area under the graphof f . If f(x) = 1, the integral is the length of the interval. The function F (x) =Rxaf(y) dy is calledan anti-derivative of f. The fundamental theorem of calculus states F0(x) = f (x). Unlike the derivative,anti-derivatives can not always be expressed in terms of known functions: Example: F (x) =Rx0e−x2dx. Of-ten, the anti-derivative can be found: Example: f(x) = sin2(x) = (cos(2x) + 1)/2, F (x) = x/2 − sin(2x)/4.AVERAGES=MEAN. www.worldclimate.com gives the follow-ing data for the average monthly rainfall (in mm) for Cam-bridge, MA, USA (42.38 North 71.11 West,18m Height).Jan Feb Mar Apr May Jun Jul Aug Sep Oct Nov Dec93.9 88.6 83.3 67.0 42.9 26.4 27.9 83.8 35.5 61.4 166.8 82.8The average 860.3/12 = 71.7 is a Rieman sum integral.1 2 3 4 5 6 7 8 9 10 11 122550751001251502D INTEGRATION. If f(x, y) is a continuous function of two variables on a region R, the integralRRf(x, y) dxdy can be defined as the limit1n2Pi,j,xi,j∈Rf(xi, yj) with xi,j= (i/n, j/n) when n goes toinfinity. This integral divided by the area is the average value of f on the region R. If f(x, y) = 1, thenthe integral is the area of the region R. For many regions, the integral can be calculated as a double in-tegralRba[Rd(x)c(x)f(x, y) dy]dx. In general, the region must be split into pieces, then integrated seperately.EXAMPLE. CalculateRRf(x, y) dxdy, where f(x, y) = 4x2y3and where R is the rectangle [0, 1] × [0, 2].Z10[Z204x2y3dy] dx =Z10[x2y4|20] dx =Z10x2(16 − 0) dx = 16x3/3|10=163.TYPES OF REGIONS.R RRf dA =RbaRg2(x)g1(x)f(x, y) dydx type I region.R RRf dA =RbaRh2(y)h1(y)f(x, y) dxdy type II region.R RRf(x, y)dxdy =RβαRbaf(r cos(θ), r sin(θ)) rdrdθ integral in polar coordinates.EXAMPLE. Let R be the triangle 1 ≥ x ≥ 0, 1 ≥ y ≥ 0, y ≤ x. CalculateRRe−x2dxdy.ATTEMPT.R10[R1ye−x2dx]dy. We can not solve the inner integral because e−x2has no anti-derivative in terms of elementary functions.IDEA. Switch order:R10[Rx0e−x2dy] dx =R10xe−x2dx = −e−x22|10=(1−e−1)2=0.316....If you can’t solve adouble integral, try tochange the order of in-tegration!A special case of switching the order of integration is Fubini’s theorem:RbaRdcf(x, y) dxdy =RdcRbaf(y, x) dydx.QUANTUM MECHANICS. In quantum mechanics, the motion of a particle (like an electron) in the plane isdetermined by a function u(x, y), the wave function. Unlike in classical mechanics, the position of a particleis given in a probabilistic way only. If R is a region and u is normalized so thatR|u|2dxdy = 1, thenRR|u(x, y)|2dxdy is the probability, that the particle is in R.EXAMPLE. Unlike a classical particle, a quantum particle in a box [0, π]×[0, π] can have a discrete set of energiesonly. This is the reason for the name ”quantum”. If −(uxx+uyy) = λu, then a particle of mass m has the energyE = λ¯h2/2m. A function u(x, y) = sin(kx) sin(ny) represents a particle of energy (k2+ n2)¯h2/(2m). Our aim isto find the probability that the particle with energy 13¯h2/(2m) is in the middle 9’th R = [π/3, 2π/3]×[π/3, 2π/3]of the box.SOLUTION: We first have to normalize u2(x, y) = sin2(2x) sin2(3y), sothat the average over the whole square is 1:A =Zπ0Zπ0sin2(2x) sin2(3y) dxdy .To calculate this integral, we first determine the inner integralRπ0sin2(2x) sin2(3y) dx = sin2(3y)Rπ0sin2(2x) dx =π2sin2(3y) (the fac-tor sin2(3y) is treated as a constant). Now, A =Rπ0(π/2) sin2(3y) dy =π24, so that the probability amplitude function is f (x, y) =4π2sin2(2x) sin2(3y).0123012300.10.20.30123The probability that the particle is in R is slightly smaller than 1/9:1AZRf(x, y) dxdy =4π2Z2π/3π/3Z2π/3π/3sin2(2x) sin2(3y) dxdy=4π2(4x − sin(4x))/8|2π/3π/3(6x − sin(6x))/12|2π/3π/3= 1/9 − 1/(4√3π)The probability is slightly smaller than 1/9.MOMENT OF INERTIA. Compute the kinetic energy of a square iron plate R = [−1, 1] × [−1, 1] of densityρ = 1 (about 10cm thick) rotating around its center with a 60000rpm (rounds per minute). The angular velocityspeed is ω = 2π 60000/60 = 100 2π. Because E =R RR(rω)2/2 dxdy, where r =px2+ y2, we have E = ω2I/2,where I =R RR(x2+ y2) dxdy is the moment of inertia. For the square, I = 4/3. Its energy of the plate isω24/6 = 4π210024/6Joule ∼ 0.43KW h. You can run with this energy a 60 Watt bulb for 7 hours.WHERE DO DOUBLE INTEGRALS OCCUR?- areas.- averages. Examples: average rain fall or average population in some area.- probabilities. Expectation of random variables. - quantum mechanics: probability of particle.- moment of inertiaR RR(x2+ y2)ρ(x, y)dxdy- center of mass (R RRxρ(x, y) dxdy/M,R RRyρ(x, y) dxdy/M), with M =R RRdxdy.- 1D integrals (see challenge


View Full Document

HARVARD MATH 21A - 2D INTEGRATION

Documents in this Course
PDE’s

PDE’s

2 pages

PDE's

PDE's

2 pages

Review

Review

2 pages

intro

intro

2 pages

curve

curve

2 pages

mid1

mid1

7 pages

p-1

p-1

6 pages

contour

contour

2 pages

practice1

practice1

10 pages

diffeq1

diffeq1

6 pages

TRACES

TRACES

2 pages

PDE's

PDE's

2 pages

Review

Review

108 pages

GRAPHS

GRAPHS

2 pages

Review

Review

4 pages

VECTORS

VECTORS

2 pages

Load more
Download 2D INTEGRATION
Our administrator received your request to download this document. We will send you the file to your email shortly.
Loading Unlocking...
Login

Join to view 2D INTEGRATION and access 3M+ class-specific study document.

or
We will never post anything without your permission.
Don't have an account?
Sign Up

Join to view 2D INTEGRATION 2 2 and access 3M+ class-specific study document.

or

By creating an account you agree to our Privacy Policy and Terms Of Use

Already a member?