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All the way from Unit 1 to Unit 4

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1 All the way from Unit 1 to Unit 4
Diff Eq Final Review All the way from Unit 1 to Unit 4

2 Easiest Point-Verifying a diff eq
This simply plug and chug, making sure both sides are equal Take the 1st and 2nd derivative and plug all into the diff eq Ex: Verify 𝑦 𝑑 = 6 5 βˆ’ 6 5 𝑒 βˆ’20𝑑 𝑖𝑠 π‘Ž π‘ π‘œπ‘™π‘’π‘‘π‘–π‘œπ‘› π‘‘π‘œ 𝑑𝑦 𝑑𝑑 +20𝑦=24 Take the derivatives, 1st : y’(t)=24 𝑒 βˆ’20𝑑 , no need for the 2nd Plug into the original equation 24 𝑒 βˆ’20𝑑 +20( 6 5 βˆ’ 6 5 𝑒 βˆ’20𝑑 )=24 Simplify: 24 𝑒 βˆ’20𝑑 +24βˆ’24 𝑒 βˆ’20𝑑 )=24 So 24=24

3 Our ways to solve a diff eq A SINGLE DIFF EQ

4 These are The main Things to know Solving a diff eq Unit 1 Homogenous
Phase Portraits Non-Homogenous Linear and Separation of Variables Exact Equations Unit 2 No RHS (It is = to 0) 3 possible solutions RHS (There is a driving force) Method of Undetermined Coefficents Variation of Parameters Unit 3 Solving through laplace transforms Unit Step Functions Dirac Delta Functions These are The main Things to know

5 Unit 1-The Phase Portrait
If the equation is y(assuming the dependent variable) (squared, cubed, multiplied, plus) =0 Factor-Find zeros Graph the zeros on the number line Figure out the signs in between, find attractors and repellers Now graph the solution, attractors and repellers Repeller Attractor Attractor Repeller

6 Unit 1- 3 forms of solving the equation
Separation of variables When u can move everything with x to one side and everything with y to the other side, then take the integral of both sides After taking the integral Explicit (solve for y) Implicit (Don’t worry Linear When the equation is in a very distinct form or can be manipulated into that form Exact See if u can change into that formula Then check to see if it is exact Than take 2 integrals

7 Separation of variables
Know how to do IBP, u-sub and basic trig integrals Process Move everything with x and everything with y to each side Leave 𝑑𝑦 𝑑π‘₯ on the side with the y’s Multiply by dx 𝑑𝑦 𝑑π‘₯ 𝑦 𝑠𝑑𝑒𝑓𝑓 = π‘₯ 𝑠𝑑𝑒𝑓𝑓 = 𝑑𝑦 𝑦 𝑠𝑑𝑒𝑓𝑓 =(𝑑π‘₯)(π‘₯ 𝑠𝑑𝑒𝑓𝑓) Take the integral of both sides 𝑦 𝑠𝑑𝑒𝑓𝑓 𝑑𝑦 = π‘₯ 𝑠𝑑𝑒𝑓𝑓 𝑑π‘₯ If it asks for the implicit leave it as is, if it asks for the explicit solution you have to solve for y in terms of x

8 The linear Case Where p(x) and q(x) are y as a function of x
Meaning you will only see x’s Get into the following Form in you can 2. Find the integrating factor 3. Multiply by the integrating factor 𝑑 𝑑π‘₯ 𝑦 πΌπ‘›π‘‘π‘’π‘”π‘Ÿπ‘Žπ‘‘π‘–π‘›π‘” π‘“π‘Žπ‘π‘‘π‘œπ‘Ÿ =RHS(Integrating factor) 4. Integrate both sides 𝑑 𝑑π‘₯ 𝑦 πΌπ‘›π‘‘π‘’π‘”π‘Ÿπ‘Žπ‘‘π‘–π‘›π‘” π‘“π‘Žπ‘π‘‘π‘œπ‘Ÿ 𝑑π‘₯= 𝑅𝐻𝑆 πΌπ‘›π‘‘π‘’π‘”π‘Ÿπ‘Žπ‘‘π‘–π‘›π‘” π‘“π‘Žπ‘π‘‘π‘œπ‘Ÿ 𝑑π‘₯ 5. The LHS simply becomes (y)(Integrating factor)= 𝑹𝑯𝑺 π‘°π’π’•π’†π’ˆπ’“π’‚π’•π’Šπ’π’ˆ 𝒇𝒂𝒄𝒕𝒐𝒓 𝒅𝒙 6. Now take the integral and solve for y if it asks for the explicit solution

9 The exact case Where M and N can be functions of x and y
Remember when taking partials, treat the Other variable as a constant Ex: 𝑑 𝑑π‘₯ 2π‘₯ =π‘₯ so 𝑑 𝑑π‘₯ π‘₯𝑦 =π‘₯ 𝑑 𝑑π‘₯ 2 = so 𝑑 𝑑π‘₯ 𝑦 =0 Notice very distinct difference Exact equations look like Make sure the equation is exact by checking Take 2 integrals (Don’t forget the plus C) In this case 𝑀𝑑π‘₯ =𝑆𝑑𝑒𝑓𝑓+𝒇(π’š) And 𝑁𝑑𝑦 =𝑆𝑑𝑒𝑓𝑓+π’ˆ(𝒙) 4. Now go on hunt and combine the 2 integrals a. Pick one of the integrals and grab f(x) or g(y) from the other Same story on partials here 3π‘₯𝑑π‘₯ =3( π‘₯ 2 2 ) π‘₯𝑦𝑑π‘₯ =𝑦( π‘₯ 2 2 ) Need 𝑀𝑑π‘₯ and 𝑁𝑑𝑦 Ex: That’s say you get the following out of the integrals 𝑓 π‘₯,𝑦 = π‘₯ 2 𝑦+ 𝑦 2 +𝒇 𝒙 𝑓 π‘₯,𝑦 = π‘₯ 2 𝑦+π₯𝐧 𝐱 +g(y) Ans: 𝑓 π‘₯,𝑦 = π‘₯ 2 𝑦+ 𝑦 2 +ln⁑(π‘₯)

10 The 3 possible solutions
Come from the Characteristic Equation

11

12

13 Variation of parameters For Martin-Formulas is given
Kumudu-The Determinants

14 UNIT 4-SOLVING SYSTEMS OF EQUATIONS

15 Write in general matrix form
Apply the identity Or use… Write in the general solution form (This assumes 2 real roots) Use the following idea to solve for the coefficients Apply for both the eigenvalues to solve for the 2 eigen vectors When you solve this, you will get 2 equations, you can pick either one, and This will tell you a relationship between k1 and k2, set k1=0 and solve for k2 Put into the vector 𝐾 1 𝐾 2 , this is the eigenvector to correspond with the πœ†

16 𝑑𝑒𝑑𝐴>0, π‘‘π‘Ÿπ΄<0 (π‘‘π‘Ÿπ΄) 2 <4𝑑𝑒𝑑𝐴 𝑑𝑒𝑑𝐴>0, π‘‘π‘Ÿπ΄>0 (π‘‘π‘Ÿπ΄) 2 <4𝑑𝑒𝑑𝐴 𝑑𝑒𝑑𝐴>0, π‘‘π‘Ÿπ΄>0 (π‘‘π‘Ÿπ΄) 2 >4𝑑𝑒𝑑𝐴 𝑑𝑒𝑑𝐴>0, π‘‘π‘Ÿπ΄<0 (π‘‘π‘Ÿπ΄) 2 >4𝑑𝑒𝑑𝐴 𝑑𝑒𝑑𝐴<0

17 Unit 1 You can only use the method for linear if the equation can be put into that form In solving linear, remember to multiply the and RHS and LHS by the integrating factor You can factor out, divide and multiply to separate variables, but be careful! 𝑦 2 π‘₯βˆ’π‘¦, π‘¦π‘œπ‘’ 𝒄𝒂𝒏𝒏𝒐𝒕 π‘“π‘Žπ‘π‘‘π‘œπ‘Ÿ π‘œπ‘’π‘‘ π‘‘β„Žπ‘’ 𝑦 π‘π‘’π‘π‘Žπ‘’π‘ π‘’ 𝑦 2 π‘₯βˆ’π‘¦=𝑦 π‘₯π‘¦βˆ’1 , π‘₯,𝑦 still trapped together Unit 2 If the Guess matches the general solution, modify by multiplying by x Remember to keep the nature (exponent in a e, argument in a sin or cos), when making a guess on the RHS For variation of parameters, it should be a simple integral you are left with Unit 3 Remember the tricks for unit step functions and dirac delta functions Both unit step functions and dirac delta functions in the original should lead to an answer with a unit step Remember laplace in the beginning, algebraically rearrange, then take the inverse laplace Unit 4 Really study the chart corresponding to the different possibilities Remember the difference between a stable and unstable node and what makes each Know the process of how to get the eigenvectors and don’t forget they are vectors, so u need both components, set 1 comp. = to 1, use relation to find the other


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