Differential Equations Compute y’ and y’’ and then combine these derivatives with y as a linear second-order differential equation that is free of the symbols c1 and c2 and has the form F(y, y’, y’’)=0. The symbols c1 and c2 represent constants. Y= c1ex + c2xex Verify that the indicated function is a particular solution of the given differential equation. Give an interval of definition I for each solution. y’’ + y = sexx; y=xsinx + (cosx)ln(cosx) Solve the differential equation (2x+y+1)y’ =1 Solve the given initial-value problem and give the largest interval I on which the solution is defined. dy/dt + 2(t+1)y2 = 0, y(0) = -1/8 According to Stefan’s law of radiation the absolute temperature T of a body cooling in a medium at constant absolute temperature Tm is given by dT/dt = k(T4 – T4m), solve the differential equation. Using the information provided in problem #5, show that when T-Tm is small in comparison to Tm then Newton’s law of cooling approximates Stefan’s law. Find the general solution of the differential equation. 2y’’ + 2y’ +3y =0 Solve the differential equation subject to the indicated conditions. Y’’ + 2y’ +y=0, y(-1) = 0, y’(0) = 0 Amass weighing 32 pounds stretches a spring 6 inches. The mass moves thought a medium offering a damping force that is numerically equal to ? times the instantaneous velocity. Determine the values of ? >0 for which the spring? Mass system will exhibit oscillatory motion. The vertical motion of a mass attached to a spring is describe by the IVP 1/4x’’ + x’ + x = 0, x(0)=4, x’(0)=2. Determine the maximum vertical displacement of the mass.
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