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Condenser Oscillation Frequency and Decrement

For the oscillating condenser case, Steinmetz gives the frequency of oscillation in the form:

f=12π1LC(r2L)2f = \frac{1}{2\pi}\sqrt{\frac{1}{LC} - \left(\frac{r}{2L}\right)^2}

For negligible resistance, this reduces to:

f=12πLCf = \frac{1}{2\pi\sqrt{LC}}

The critical resistance condition appears as:

r12=4LCr_1^2 = \frac{4L}{C}

For the decrement of oscillation, Steinmetz relates the amplitude ratio of successive half waves to resistance:

Δ=eδ\Delta = e^{-\delta} δ=π(r1r)21\delta = \frac{\pi}{\sqrt{\left(\frac{r_1}{r}\right)^2 - 1}}
Original scan crop of Steinmetz Fig. 14 oscillating condenser charge
Fig. 14

Oscillating condenser charge with decaying current and potential waves.

Original scan crop of Steinmetz Fig. 15 decrement of oscillation
Fig. 15

Decrement as a function of actual resistance divided by critical resistance.

Modern redraw sheet for Steinmetz condenser response figures
Redraw sheet

Modern visual guide for the equation family; not a substitute for the original figures.

SymbolSteinmetz ContextModern Reading
rResistance of the circuit.Series resistance.
LInductance.Inductance.
CCapacity of the condenser.Capacitance.
r_1Critical resistance.Boundary between oscillatory and non-oscillatory response.
DeltaAmplitude ratio of successive half waves.Decrement or decay ratio.

The frequency formula shows that resistance lowers the oscillation frequency and reaches zero at the critical boundary. The decrement formula shows how rapidly the oscillation fades once it exists.

In plain language: inductance and capacity make oscillation possible, while resistance decides how much of that oscillation survives from one half wave to the next.

Use the Transient RLC Response tool to vary r, L, and C while watching the transition between oscillatory discharge, critical damping, and non-oscillatory discharge. The tool reports the critical resistance and half-wave ratio so the modern curve can be compared with Steinmetz’s decrement discussion.

Modern Electrical Engineering Interpretation

Modern readers can recognize these equations as underdamped series RLC behavior. The important historical value is that Steinmetz frames the result through condenser charge, critical resistance, and decrement rather than only through later normalized damping terminology.

Interpretive Reading

Interpretive only: the equations make energy exchange between magnetic and electrostatic storage visible. A field-language reading may emphasize that the oscillation is not a motion of particles through a passive mathematical abstraction, but a timed exchange between stored field states. That statement is interpretive, while the equations and figures are source-grounded.

Steinmetz’s plotted examples use values such as L = 100 mh. and C = 10 mf. in the figure captions. The archive should preserve those printed units, then separately translate them into modern unit conventions after source verification.

  • Exact exponent signs and OCR-sensitive symbols around equations 48-62.
  • Edition-specific typography for Delta, delta, and critical resistance.
  • Unit normalization for mh. and mf. in the examples.