There are voltage drops based on Q, dQ/dt, and d(dQ/dt); what about d(d(dQ/dt))?

  • Thread starter Thread starter kmarinas86
  • Start date Start date
  • Tags Tags
    Voltage
AI Thread Summary
The discussion explores the concept of voltage drops in electrical circuits, identifying that capacitive drops relate to charge (Q), resistive drops to the rate of charge change (dQ/dt), and inductive drops to the acceleration of charge change (d(dQ/dt)). It raises the question of whether a fourth type of voltage drop exists that corresponds to the third derivative of charge with respect to time (d(d(dQ/dt))), suggesting a potential resistance to changes in acceleration of charge. The analogy of vehicle acceleration is used to illustrate how different systems respond to changes in input, implying that there could be parameters affecting these "opposing electric fields." The discussion concludes by noting that no physical device has been observed to produce a voltage drop proportional to the third derivative of charge, leaving the existence of such a phenomenon open to speculation. Overall, the inquiry highlights the need for further exploration into the nature of voltage drops beyond the established categories.
kmarinas86
Messages
974
Reaction score
1
Capacitive voltage drops are based on Q.
Resistive voltage drops are based on dQ/dt.
Inductive voltage drops are based on d(dQ/dt).

However, wouldn't there be a logical progression from here? Isn't there a voltage drop for d(d(dQ/dt)), that is to say, some kind of property of the circuit that resists alterations in the acceleration of charge?

Think of it this way:

Capacitance is to position, in the same way that
Resistance is to motion, in the same way that
Inductance is to acceleration, in the same way that
? is to changes in acceleration

This can be likened to how the various results one may get from different vehicles depending on how hard and swifly one presses the power pedal. Alternatively, it can looked upon this way:

1) Some cars will build their acceleration almost instantaneously (e.g. electric cars).
2) Others will take more time to get that same acceleration (e.g. equivalent gasoline-powered cars).

I'd imagine that if a charge is prevented from accelerating, there must be something to act against that acceleration. But this can go both ways to where if a charge is prevented from additional deceleration, then something may act against that deceleration. It would be as though a opposing field were generated simultaneously (but not equally matching) upon the application of a field of opposite polarity. So would the various conditions that determine the rate change and the acceleration of rate change of the presence of these "opposing electric fields" be parameters underlying "other" voltage drops unique from V_R, V_L, and V_C? The fourth one, in particular, would analogous to "mechanical impedance", where a smooth application of torque on a motor may result not in long term angular acceleration but simply an accumulated drop in angular velocity (while the introduction of that torque would be what is necessary to cause that angular acceleration). However, would such voltage drops be separate from resistive, inductive, and capacitive voltage drops, or are those three categories of voltage drops already inclusive of these considerations?

If a "fourth" voltage drop such as this doesn't exist, what is the theory behind that conclusion?
 
Last edited:
Physics news on Phys.org
As far as I know, it's simply because no physical device has ever been observed that produces a voltage drop proportional to \mathrm{d}^3 Q/\mathrm{d}t^3 (or any higher derivative). I can't think of any physical reason why one couldn't exist. But I'm not an expert on circuit components.
 
This is from Griffiths' Electrodynamics, 3rd edition, page 352. I am trying to calculate the divergence of the Maxwell stress tensor. The tensor is given as ##T_{ij} =\epsilon_0 (E_iE_j-\frac 1 2 \delta_{ij} E^2)+\frac 1 {\mu_0}(B_iB_j-\frac 1 2 \delta_{ij} B^2)##. To make things easier, I just want to focus on the part with the electrical field, i.e. I want to find the divergence of ##E_{ij}=E_iE_j-\frac 1 2 \delta_{ij}E^2##. In matrix form, this tensor should look like this...
Thread 'Applying the Gauss (1835) formula for force between 2 parallel DC currents'
Please can anyone either:- (1) point me to a derivation of the perpendicular force (Fy) between two very long parallel wires carrying steady currents utilising the formula of Gauss for the force F along the line r between 2 charges? Or alternatively (2) point out where I have gone wrong in my method? I am having problems with calculating the direction and magnitude of the force as expected from modern (Biot-Savart-Maxwell-Lorentz) formula. Here is my method and results so far:- This...
Back
Top