That helps a lot; you didn't mean what you wrote (or rather, what I read)! I was thinking of "\(dx^2\)" as "\((dx)^2\)", or "\(dxdx\)" as in \(\frac{d^2y}{dx^2}\). That would have made this a double integral, and your notation would be quite odd.
You are thinking instead of \(d(x^2)\), the differential of the function \(y = x^2\). In this sense, \(dy = 2x dx\). So \(\int x^2d(x^2)=\int x^2\cdot 2x dx=\int 2x^3 dx=\frac{1}{2}x^4 + C\).
And in fact, it could have been expressed simply as \(\int y dy=\frac{1}{2}y^2 + C=\frac{1}{2}x^4 + C\).
You may well get an answer from a physics perspective; but it may help if you tell us more about the context in which you found this.
Well, thank you, that cleared my ideas a lot.
But I am still not getting the sense of writing something like [MATH]g(x) = f(x)dx[/MATH].
Is [MATH]g(x)[/MATH] equal to [MATH]\int f(x)dx[/MATH]?
Or does it is have a different meaning?
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Ok, I've been thinking about it pretty much and maybe it makes sense now.
That just means what I see, a function for the differential of a variable, which actually isn't an integral.
The integration operation "automatically" multiplies the differential, then it's wrong to say for example [MATH]f(x) = x^2dx = 2x[/MATH], instead, it is true to say [MATH]df(x) = x^2dx[/MATH] and therefore [MATH]f(x) = 2x[/MATH] like a normal differential equation.
Am I right?
Here's where I found it:
There was this slide about the work of a force that showed how to get the formula [MATH]dW = \frac1 2 md(v^2)[/MATH] where W is the work, m is the mass and v is the speed.
The steps were:
Given that [MATH]dW = F\cdot dr[/MATH],
[MATH]dW = F\cdot dr = F\cdot vdt = m\frac{dv}{dt}\cdot vdt = m\cdot vdv[/MATH] where t is the time;
if [MATH]d(v^2) = 2vdv[/MATH] then [MATH]dW = \frac 1 2 md(v^2)[/MATH]Which didn't make much sense to me at the beginning because [MATH]dW[/MATH] was notated as [MATH]\delta W[/MATH] and I didn't realize that it was just a normal differential.
To conclude, if you divide both sides for [MATH]dp[/MATH] where p is the variable of the position in space, and then integrate both sides for p:
[MATH]\int_{p_1}^{p_2} \frac {dW}{dp}dp = \int_{p_1}^{p_2}\frac 1 2 m\frac {d(v^2)}{dp}dp[/MATH] (yeah, it's just a normal integration but to be complete I also divided by [MATH]dp[/MATH])
i get
[MATH]W(p_2)-W(p_1) = \frac 1 2 m(v(p_2))^2 - \frac 1 2 m(v(p_1))^2[/MATH].
So if I name [MATH]E_k(p) = \frac 1 2 m(v(p))^2[/MATH] the kinetic energy, that equation shows that the work made by a force is the difference of the kinetic energy of the object in the positions:
[MATH]W(p_2)-W(p_1) = E_k(p_2) - E_k(p_1)[/MATH]