Kronecker Delta and Things (Term 2) Flashcards

1
Q

What is the integral from 0 to L of sin(nπx/L)*sin(mπx/L) dx equal to?

A

L/2 * δnm, where δnm is the kronecker delta, which equals 1 if n=m and 0 otherwise

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2
Q

What can we do with the kronecker delta form of the integral?

A

Substitute it into the integral equation from before (orthogonality thing) and get rid of the sum (change n for m

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3
Q

What is the equation for Cn?

A

Cn = 2/L * integral between 0 and L of f(x)*sin(mπx/L) dx

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4
Q

How do you work out the final equation for u(x,t)?

A

-Split the integral into 2 part (0 to L/2 and rest) and substitute in f(x) for these domains -Do the integrals to find the final value of Cn -Substitute Cn into general solution from before

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5
Q

What does u(x,t) equal finally?

A

u(x,t) = sum of 2/L * (4*E*L*sin(nπ/2))/(π^2*n^2) * sin(nπx/L)*cos(ncπt/L) (for n odd)

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6
Q

If you strike a string with hammer with head of width w, what is du(x,0)/dt

A

-0 for x < x0-w/2 -v for x0-w/2 < x < x0+w/2 -0 for x > x0 + w/2

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7
Q

What do we do to the Cn constant in the hammer problem?

A

Set them to 0, otherwise the displacement at t=0 will not vanish, so only have Dn constants this time.

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8
Q

What do we do with the initial velocity condition du(x,0)/dt = v0*δ(x-x0)?

A

-Take time derivative of u(x,t) with only Dn in and then substitute t=o in -Make this answer equal to the initial condition: v0*δ(x-x0)

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9
Q

What do we do with the initial condition after we have subbed it in?

A

-Multiply both sides by sin(mπx/L) and integrate again, and rearrange to get the orthogonality relationship.

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10
Q

What is the orthogonality relationship and what does it equal?

A

integral from 0 to L of sin(nπx/L)*sin(mπx/L) = L/2*δnm

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11
Q

What do we do after using the orthogonality relationship in the hammer problem?

A

Find Dm by taking the sum out and the kronecker delta out (n=m), and rearrange for Dm.

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12
Q

How do you do separation of variables for the diffusion equation?

A

u(x,t) = X(x)T(t), and sub this in. Then move around until same variables on same side, and set equal to lambda, a constant.

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13
Q

What happens when lambda = 0 for the diffusion equation?

A

-d^2X/dx^2 = 0, so X(x) = A0x+ -dT/dt = 0, so T(t) = G0 -Therefore u(x,t) = (A0x+B0)*G0 = A0’x+B0’

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14
Q

For the diffusion solution when lambda = 0, when are the equilibrium and steady-state solutions?

A

-Equilibrium when u(x,t) = B0 -Steady-state when u(x,t) = A0x+B0 (A0 not equal to zero)

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15
Q

How can you maintain the steady state? What is the flux equal to?

A

Feed particles in at the left and pull them out on the right with exactly the right rate. Flux j=-D du(x,t)/dx

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16
Q

How do you work out the equation for λ?

A
  • Relabel m to n in the equation for Dm, and sub this new Dn into u(x,t)
  • Set this new equation equal to v0*sin(πx/L)
  • Only D1 is not equal to zero, so rearrange this and find u(x,t) = v0L/cπ * sin(πx/L)*sin(cπt/L)
  • Only have one pure frequency ω = cπ/L, so λ = 2L
17
Q

What happens when lambda > 0 (lambda = k^2) for the diffusion equation?

A

-dT/dt = D*k^2*T(t) -Solution is T(t) = G*e^(D*k^2*t) -Not physical as t goes to 0, so exclude this choice

18
Q

What happens when lambda < 0 (lambda = -k^2)?

A

-Both sides equal -k^2 -T(t) = G*e^(D*k^2*t) again -X(x) = Ak*cos(kx)+Bk*sin(kx)

19
Q

What is the final solution for the diffusion equation?

A

u(x,t) = sum over k of (Ak*cos(kx)+Bk*sin(kx))*exp(-D*k^2*t) + A0+B0x

20
Q

What do we do if we specify boundary conditions of u(x=0,t)=u(x=L,t)=0 for the diffusion equation general solution? (lasers which bleach dye molecules at each end)

A

-Substitute in x=0 and x=L and find the values of Ak and k from this. -Substitute thee new values in

21
Q

What if there are no lasers? What do we do to work out the solution?

A

-No flux at ends (j=0) -Take x-derivative of solution and sub in x=0 and x=L -These must both equal zero so find Bk and k values from this -Sub back in

22
Q

What is A0 equal to in the general solution?

A

A0 = N/L (equilibrium concentration)