#$&* course MTH-279 08/06 around 3:00 PM Query 27 Differential Equations*********************************************
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Given Solution: [see my note at end for correct (?) solution ] [tilson] matrix is [3, 1; -2, 1] Assume the solution will take the form y(t) = e^(λt)x, so y’ = λe^(λt)x, λe^(λt)x = Ae^(λt)x, e^(λt)(λx) = e^(λt)(Ax), λx = Ax, (A-λI)x = 0, x ≠ 0. det([3-λ, 1; -2, 1-λ]) = 0 λ^2 - 4λ + 5 = 0 λ = 2 ± i For λ = 2 + i: [3-2-i, 1; -2, 1-2-i] = [1-i, 1; -2, -1-i]. Using row reduction, we get [2, 1+i; 0,0]. This can be interpreted as 2x + (1+i)y = 0. Putting this into vector form, we get: v_1=[-1-i; 2]. For λ = 2-i: [3-2+i, 1; -2, 1-2+i] = [i+i, 1; -2, -1+i]. Using row reduction, we get [2, 1-i; 0, 0]. This can be interpreted as 2x + (1-i)y = 0. Putting this into vector form, we get: v_2 = [-1+i; 2]. [white] Phi = [-4 +5e^t , 4 - 4e^t ; -5+5e^t , 5-4e^t] y(3) = [e^2 + 1 ; e^2] using the fact that e^(tA) = T*lam*T_inv I found my evals to be 0 and 1 and my evecs to be [4 ; 5] and [1 ; 1] so T = [4 , 1 ; 5 , 1] T_inv = [-1 , 1 ; 5 , -4] I then computed [4 , 1 ; 5 , 1]*[1 , 0 ; 0 , e^t]*[-1 , 1 ; 5 , -4] = [-4 +5e^t , 4 - 4e^t ; -5+5e^t , 5-4e^t] to find y(3), I set up [-4 +5e^(t-s) , 4 - 4e^(t-s) ; -5+5e^(t-s) , 5-4e^(t-s)] = [y_t1 - y_s1 ; y_t2 - y_s2] or [-4 +5e^2 , 4 - 4e^2 ; -5+5e^2 , 5-4e^2] = [ y_t1 - 1 ; y_t2 + 0] and solved for y. [my note]
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Given Solution: &&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&& Self-critique (if necessary): Self-critique rating: ********************************************* Question: Solve the equation y ' = [0, -9; 1, 0] y with initial condition y(0) = [6, 2]. YYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYY Your solution: remember y’ = Alambda p(lambda) = det [A - lambda I] = 0 --follow the steps similar to those in problem one— we find lambda = +/- 3i --now solve for the eigenvectors— using [A - lambda1 I] * x1vector = [0;0] and [-3i, -9 ; 1 , -3i] * [x1; x2] = [0;0] for reference x2 = 1/3 and x1 = i, so x1vector = [i; 1/3] same method shows that x2vector = [-i; 1/3] y1(t) = e ^ 3it [ i 1/3] y1(t) = [ie^3it ; 1/3 e^3it] --- y2(t) = e^-3it [-i; 1/3] y2(t) = [-ie^-3it; 1/3 e^-3it] --- y(t) = c1y1(t) + c2y2(t) = [ie^3it , -ie^-3it ; 1/3e^3it , 1/3 e^-3it] * [c1; c2] --- w(t) = det [above matrix w/ zero plugged in] =det[i, -i ; 1/3, 1/3] =(i * 1/3) - (1/3 * -i) = 1/3i + 1/3i = 2/3i w(t) does not equal zero --- y(0) = [i , -i ; 1/3, 1/3] * [c1; c2] = [6;2] distribute and rearrange [c1; c2] = [3i + 3; -3i + 3] -- y(t) = 3i + 3 [ie^3it; 1/3 e^3it] -3i + 3 [ -ie^-3it ; 1/3 e^-3it] Confidence rating: 2,3
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Given Solution: &&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&& Self-critique (if necessary): OK Self-critique rating: OK ********************************************* Question: Find all values of mu such that any fundamental set [ y_1, y_2 ] of the system y ' = [1, 3; mu, -2] y has the property that the limit of the expression (y_1(t))^2 + (y_2(t))^2, as t -> infinity, is zero. [tilson] lim(e^(-(t^2))) as t ∞ = 0. As long as the solution takes a form of e^(-(t^2)), the limit will be 0. In order to get a solution that will take that form when squared, we’re looking for complex eigenvalues, since (±i)^2 = -1. It doesn’t really matter if we have the positive or negative eigenvalue, as long as it is complex. We find the eigenvalues as normal, det([1-λ, 3; µ, -2-λ]) = 0, λ^2 + λ - (3µ + 2) = 0. Using the quadratic formula, we get: -1/2 ± sqrt(9+12µ)/2. We know that we need the sqrt()/2 term to equal a multiple of i. Knowing this, we set up an equality: sqrt(9+12µ)/2 = ni. Solving, we get µ = -n^2/3 - 3/4. This means that n can be any real value. In that regard, µ can take any value such that -12µ is greater than 9.
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Given Solution: &&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&& Self-critique (if necessary): Self-critique rating: ********************************************* Question: A particle moves in an unspecified force field in such a way that its position vector r(t) = x(t) i + y(t) j and the corresponding velocity vector v(t) = r ' (t) satisfy the equation v ' = 2 k X v Write this condition as a system v ' = A v, with v = [v_x; v_y]. YYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYY Your solution: Confidence rating: \Given Solution: A particle moves in an unspecified force field in such a way that its position vector r(t) = x(t) i + y(t) j and the corresponding velocity vector v(t) = r ' (t) satisfy the equation v ' = 2 k X v Write this condition as a system v ' = A v, with v = [v_x; v_y]. I’m a bit stumped by this problem. The X in v’ = 2kXv is throwing me off. I’m not sure if that’s supposed to indicate the cross product, as in “2k crossed with v”, or if X is intended to be a separate matrix, or if 2k is even supposed to represent 2 units in the k direction. Since you’ve used i and j to denote directions in r(t), I’m assuming that k is the k direction. But the X is still throwing me off. I’ll just assume that it’s “2k crossed with v.” @& That is the correct assumption. *@ [0,0,2]x[v_x, v_y, v_z] = [-2v_y, 2v_x], v’ = [0, -2; 2, 0][v_x; v_y], @& Good, but [v_x ' ; v_y '] = [0, -2; 2,0] [v_x; v_y] would be more explicit v ' = [0, -2; 2, 0] v is another alternative. @ det([-λ, -2; 2, -λ]) = 0, λ^2 + 4 = 0, λ = ±2i. For λ = -2i: [2i, -2; 2, 2i]. Using row reduction, we get: [1, i; 0, 0]. We interpret this as x+iy=0. We translate this into vector form as v_1 = [1; i]. @& fine, but maybe [v_x; v_y] = [1; i] to emphasize the details @ v(t) = e^(-2it)[1;i] = (cos(2t) - i*sin(2t))[1;i] = u + iv = [cos(2t); sin(2t)] + i[-sin(2t); cos(2t)] v(t) = c_1[cos(2t); sin(2t)] + c_2[-sin(2t);cos(2t)] v(0) = [c_1cos(0) - c_2sin(0); c_1sin(2t) + c_2cos(2t)] = [1;2], c_1 = 1, c_2 = 2. r(t) = ʃv(t)dt = [cos(2t) + sin(2t)/2 + c_3; sin(2t) - cos(2t)/2 + c_4]. r(0) = [1+c_3; c_4 - ˝] = [2; 1]. c_3 = 1, c_4 = 3/2. r(t) = [cos(2t) + sin(2t)/2 + 1; sin(2t) - cos(2t)/2 + 3/2] r(3π/2) = [0; 2]. The particle’s position is 2j. &&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&& Self-critique (if necessary): Self-critique rating: " Self-critique (if necessary): ------------------------------------------------ Self-critique rating: " Self-critique (if necessary): ------------------------------------------------ Self-critique rating: #*&!