Differential and derivatives [HELP]

AI Thread Summary
Differentials and derivatives are fundamental concepts in calculus, used to describe small changes in variables, such as dV representing an infinitesimally small change in volume. In dynamics and thermodynamics, these concepts help in formulating equations like dA = Fdr and PdV, where the focus is on the limits of these small changes rather than their exact values. The notation a = d²r/dt² is a concise way to express acceleration as the second derivative of position with respect to time, while the dots indicate first and second derivatives. Understanding these principles is crucial for applying calculus in physics, particularly in analyzing work done along a path. Resources like MIT courses can provide further clarification on these topics.
xmedium
Messages
2
Reaction score
0
Can someone explain to me what are differential and derivatives used for (intergrals ?) in some well known stuff from dynamics or thermodynamics:

dA=Fdr or in thermodynamics PdV

For example what is that dV ... why not just V.

Why do I sometimes write a=d^2r/dt^2 instead of a=r(:)/t(.)

(':' 2nd derivate and '.' is first derivate ------ so sorry for the input I am in a rush)

Thanks.
 
Physics news on Phys.org
The dots are just a shorthand notation, there is no difference.

dV is a small amount of V. How small? The smallest possible. The exact amount does not need to be known in the context of differential equations.

This is known as "the calculus". There are many notes and courses on the subject.
 
Im watching now someMIT courses ... is there something similar for this coz I don't really understand what "smallest possible" Work(A) might be :)
 
Work (A) = Force (F) * Displacement (r)

If the displacement is not a straight line, then we can break the path up into a series of straight lines, and so the work is then the sum of all F*r for each r, or segment of the path. Letting this segment lengths approach zero, the sum becomes an integral and the "r's" becomes "dr's". Differentiating with respect to r, dA/dr = F , or in differential form, dA = Fdr.
 
Thread 'Gauss' law seems to imply instantaneous electric field propagation'
Imagine a charged sphere at the origin connected through an open switch to a vertical grounded wire. We wish to find an expression for the horizontal component of the electric field at a distance ##\mathbf{r}## from the sphere as it discharges. By using the Lorenz gauge condition: $$\nabla \cdot \mathbf{A} + \frac{1}{c^2}\frac{\partial \phi}{\partial t}=0\tag{1}$$ we find the following retarded solutions to the Maxwell equations If we assume that...
Thread 'A scenario of non-uniform circular motion'
(All the needed diagrams are posted below) My friend came up with the following scenario. Imagine a fixed point and a perfectly rigid rod of a certain length extending radially outwards from this fixed point(it is attached to the fixed point). To the free end of the fixed rod, an object is present and it is capable of changing it's speed(by thruster say or any convenient method. And ignore any resistance). It starts with a certain speed but say it's speed continuously increases as it goes...
Maxwell’s equations imply the following wave equation for the electric field $$\nabla^2\mathbf{E}-\frac{1}{c^2}\frac{\partial^2\mathbf{E}}{\partial t^2} = \frac{1}{\varepsilon_0}\nabla\rho+\mu_0\frac{\partial\mathbf J}{\partial t}.\tag{1}$$ I wonder if eqn.##(1)## can be split into the following transverse part $$\nabla^2\mathbf{E}_T-\frac{1}{c^2}\frac{\partial^2\mathbf{E}_T}{\partial t^2} = \mu_0\frac{\partial\mathbf{J}_T}{\partial t}\tag{2}$$ and longitudinal part...
Back
Top