Suppose that we have a function that refers to itself in its derivative or second derivitive. For example, let's say that you have a spring for which the force is directly proportional to the distance the spring has been compressed. F = -cx For simplicity's sake, mass is constant, so we can just say a = -cx The differential-form equation for this acceleration is: d^{2}x/(dt)^{2} = -cx And so the speed equation is dx/dt = v_{0} + [inte]-cx(dt) How would you solve this? Or, for a simpler equation, say that the velocity of a particle depends on its position: dx/dt = c_{1} + c_{2}x How would you solve this to get to the position function?
The exponential function is ideal for what you call "self referential" d (exp(x))/dx= x. Since cos(x)= (exp(ix)- exp(-ix))/2 and sin(x)= (exp(ix)- exp(-ix))/(2i), sine and cosine also work. In particular if d^{2}x/dt^{2}= -kx, (a "linear, homogeneous differential equation with constant coefficients") Then x(t)= C_{1}cos([sqrt](k)t)+ C_{2}sin([sqrt](k)t) where C_{1} and C_{2} can be any constants. For your second example, dx/dt= c_{1}+ c_{2}x, since this is a separable first order differential equation, we can write it in "differential form" and integrate: dx/dt= c_{1}+ c_{2}x is the same as dx/(c_{1}+ c_{2}x)= dt We can integrate the left by using the substitution u= c_{1}+ c_{2}x so du= c_{2}dx and the integral is (1/c_{2})[int](1/u)du= (1/c_{2})ln|u| or (1/c_{2})ln|c_{1}+ c_{2}x|. Integrating both sides, (1/c_{2})ln|c_{1}+ c_{2}x|= t+ C where C is the "constant of integration". Of course we can rewrite this as ln|c_{1}+ c_{2}x|= c_{2}(t+ C) and, taking the exponential of both sides, c_{1}+ c_{2}x= C' exp(c_{2}t) (C' is exp(c_{2}C) so that x is again an exponential function: x(t)= (1/c_{2})(C' exp(c_{2}t)- c_{1}).
An exponential function something to the x, such as e^{x}? And such a function has a derivitive proportional to it. d(a^{x})/dx = ln(a)*a^{x}. This doesn't work for my problem, except when the initial velocity is 0, because the addition makes it not proportional. You can't have x' = x + c for an a^{x} equation. You could have (x+c)' = x, but not x' = x + c Are those supposed to be the hyperbolic trig functions? The only difference between those and the hyperbolic trig functions that I have learned is the inclusion of i, which I am assuming is the imaginiary sqrt(-1).
AN exponential function is any function that has the variable, x, as an exponent. THE exponential function is specifically e^{x}. An exponential certainly will help with something like x'= x+ c. This is what is known as a "linear non-homogeneous differential equation with constant coefficients". The simplest way to solve it is to drop the constant, c, so as to have a homogenous equation: x'= x whose solution is, of course, x(t)= Ae^{t} (A is an arbitrary constant). Since the differential equation is linear, we can simply add that to any solution of the entire equation. To get that constant c, note that the derivative of any constant is 0 so that if x= B (a constant) x'= 0 and the equation becomes 0= B+ c. x= B= -c works. The general solution to the differential equation x'= x+ c is x(t)= Ae^{t}- c. No, those are not the hyperbolic functions, those are the standard trigonometric functions. Since (sin t)'= cos t and (cos t)'= - sin t, they satisfy the equation x"= -x. Since the hyperbolic functions can be written in terms of exponentials, they satisfy (cosh t)'= sinh t and (sinh t)'= (cosh t) and thus x"= x.