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Differential Equations
The Geometric View of ODEs
01Direction Fields and the Geometric View of ODEs02Integral Curves and the Isocline Method03Perpendicular Isoclines: The Circles of y' = -x/y04Isocline Corridors and a Trap for Solutions05Existence and Uniqueness: One Curve Through a Point06Where Existence and Uniqueness FailProblem set0/10Problem set 20/10MIT problem set0/3Practice∞
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01Euler's Method and Its Three Equations02Euler's Method by Hand: Building the Table03Convexity and the Sign of Euler's Error04First Order Error: Halve the Step, Halve the Error05Improved Euler (RK2): Averaging Two Slopes06Runge-Kutta 4 and the Price of Accuracy07Singular Points: Where Every Method FailsProblem set0/10Problem set 20/10MIT problem set0/1Practice∞
First-Order Linear Equations
01First Order Linear: Standard Form and the Sign of p02The Conduction-Diffusion Model: Newton's Law of Cooling03The Integrating Factor and the Four-Step Method04Integrating Factors: Two Mistakes and a Trick Question05Constant Coefficients: Steady State and TransientProblem set0/10Problem set 20/10MIT problem set0/1Practice∞

The Conduction-Diffusion Model: Newton's Law of Cooling

Why is Newton's law of cooling written $k(T_e - T)$ rather than $k(T - T_e)$, and why is salt diffusion the very same equation?


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Your summary note

    1. 1

      Newton's law of cooling, dTdt=k(Te−T)\frac{dT}{dt}=k(T_e-T)dtdT​=k(Te​−T)

      Set up the chamber in the bath with internal temperature TTT and external TeT_eTe​, write the equation, reproduce the sign argument that fixes the order Te−TT_e-TTe​−T and keeps the conductivity kkk positive, and add T(0)=T0T(0)=T_0T(0)=T0​.

    2. 2

      Diffusion across a semipermeable membrane, dCdt=k1(Ce−C)\frac{dC}{dt}=k_1(C_e-C)dtdC​=k1​(Ce​−C)

      Write the same model with inside concentration CCC, outside concentration CeC_eCe​ and k1>0k_1>0k1​>0, and match each symbol to its counterpart in the conduction equation.

    3. 3

      Standard linear form, with k(t)k(t)k(t) and Te(t)T_e(t)Te​(t) varying

      Rearrange the conduction equation into dTdt+kT=kTe\frac{dT}{dt}+kT=kT_edtdT​+kT=kTe​, compare it with y′+py=qy'+py=qy′+py=q, then write dTdt+k(t)T=k(t)Te(t)\frac{dT}{dt}+k(t)T=k(t)T_e(t)dtdT​+k(t)T=k(t)Te​(t) and state that this is the general first-order linear equation.

    Attempt 1 of 2