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SCIENCE · INVESTIGATE AND EXPLAIN

Separate signed reactance, phase and dissipated power

In steady sinusoidal response, derivative and integral terms appear with different phases. With a cosine convention, series impedance is Z=R+i[omega L−1/(omega C)]. This packet fixes L=1 H,C=0.25 F and source RMS voltage 6 V, while resistance stays positive. The initial transient is assumed to have decayed.

Learning outcome: Compare frequencies below, at and above 2 rad/s for two positive resistances. Retain signed phase, RMS and peak current, real/reactive/apparent power and the power-triangle check. Explain why cancellation of net reactance does not imply zero instantaneous energy in L and C.

Starting recap

Review flux integrals, linear differential equations, initial conditions, complex numbers and vector derivatives. Keep source constraints, RMS conventions and calibration roles explicit.

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Try

At omega=2 rad/s and R=2 Ω, net reactance is zero, RMS current is 3 A, peak current 3√2 A and average power 18 W. At omega=1 rad/s, X=−3 Ω, so current leads the source voltage; the negative reactive power does not mean the resistor produces energy.

Open the experiment

Predict

At omega=2 rad/s and R=2 Ω, what is average real power?

Experiment

Compare frequencies below, at and above 2 rad/s for two positive resistances. Retain signed phase, RMS and peak current, real/reactive/apparent power and the power-triangle check. Explain why cancellation of net reactance does not imply zero instantaneous energy in L and C.

Use complex impedance and an RMS power account

Worked teaching model · synthetic values · Steady sinusoidal series L1 H,C.25 F,R selected,source RMS6 V with cos convention. Reactance X=omega L−1/(omega C). Initial transients have decayed. Positive phase is voltage leading current; no ideal zero-resistance driven resonance or real apparatus.

Reset keeps your prediction, captures and practice history.

Steady RMS current versus drive frequency

RMS current (A)angular frequency (rad/s)042.9997640

Unlike graph quantities rescale independently; read units and values, not screen angles. 1: same positive resistance (solid). Joined curves show the supplied model, not additional observations.

Equivalent numerical coordinates for Steady RMS current versus drive frequency

same positive resistance

angular frequency (rad/s)RMS current (A)
0.50.772988
0.543750.8450609
0.58750.9181896
0.631250.9924285
0.6751.067822
0.718751.1444
0.76251.222179
0.806251.301156
0.851.381307
0.893751.462584
0.93751.544907
0.981251.628167
1.0251.712214
1.068751.796862
1.11251.881875
1.156251.966973
1.22.051823
1.243752.136045
1.28752.219205
1.331252.300824
1.3752.380384
1.418752.45733
1.46252.53109
1.506252.601083
1.552.666738
1.593752.727511
1.63752.782905
1.681252.832487
1.7252.875905
1.768752.9129
1.81252.943317
1.856252.967106
1.92.984324
1.943752.995127
1.98752.999764
2.031252.998559
2.0752.991898
2.118752.980214
2.16252.963971
2.206252.943646
2.252.919719
2.293752.89266
2.33752.862922
2.381252.83093
2.4252.797081
2.468752.761739
2.51252.725233
2.556252.687858
2.62.649875
2.643752.611514
2.68752.572974
2.731252.534427
2.7752.496021
2.818752.45788
2.86252.420107
2.906252.382789
2.952.345997
2.993752.309787
3.03752.274203
3.081252.23928
3.1252.205044
3.168752.171513
3.21252.138698
3.256252.106606
3.32.075238
3.343752.044592
3.38752.014663
3.431251.985442
3.4751.956921
3.518751.929087
3.56251.901927
3.606251.875428
3.651.849574
3.693751.82435
3.73751.799741
3.781251.775731
3.8251.752303
3.868751.729442
3.91251.707132
3.956251.685356
41.664101

At most 82 representative computed coordinates including endpoints; the plotted curve can use a finer grid. A table of a revealed generator is not independent measurement evidence.

Calculated quantities under the declared measurement model
QuantityValueUnit
Net reactance0ohm
Impedance magnitude2ohm
RMS current3A
Peak current4.242641A
Voltage-leading-current phase0rad
Average real power18W
Signed reactive power0var
Apparent power18VA
Power factor1ratio
Power-triangle residual0VA²

The inductor and capacitor voltage phases oppose; subtract reactances before finding impedance magnitude.

With the cos convention, Z=R+i(omega L−1/(omega C)). Current lags voltage for positive X and leads for negative X. RMS quantities give average real power Irms²R; signed reactive power Irms²X describes reversible exchange, not net dissipated watts. At omega0=2 the reactances cancel and current is 6/R, finite because R is positive. Peak current is sqrt2 times RMS, not an interchangeable label.

Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.

The inductor and capacitor voltage phases oppose; subtract reactances before finding impedance magnitude.

With the cos convention, Z=R+i(omega L−1/(omega C)). Current lags voltage for positive X and leads for negative X. RMS quantities give average real power Irms²R; signed reactive power Irms²X describes reversible exchange, not net dissipated watts. At omega0=2 the reactances cancel and current is 6/R, finite because R is positive. Peak current is sqrt2 times RMS, not an interchangeable label.

Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.

Understand

State geometry, sources and initial data

In steady sinusoidal response, derivative and integral terms appear with different phases. With a cosine convention, series impedance is Z=R+i[omega L−1/(omega C)]. This packet fixes L=1 H,C=0.25 F and source RMS voltage 6 V, while resistance stays positive. The initial transient is assumed to have decayed.

Derive the field or circuit relation

The net reactance X=omega−4/omega can be positive, zero or negative. Current RMS magnitude is 6/sqrt(R²+X²), and voltage-leading-current phase is atan2(X,R). Positive X means current lags; negative X means it leads. Subtract the opposite reactances before taking the magnitude rather than adding all three voltage magnitudes.

Audit energy, uncertainty and domain

Average dissipated power is Irms²R. Signed reactive power Irms²X describes reversible exchange, not net heat, while apparent power is VrmsIrms. At omega=2 the reactances cancel, but current remains finite because R is nonzero. Peak current is sqrt2 times RMS; mixing those conventions creates a factor-of-two power error.

Worked original case

At omega=2 rad/s and R=2 Ω, net reactance is zero, RMS current is 3 A, peak current 3√2 A and average power 18 W. At omega=1 rad/s, X=−3 Ω, so current leads the source voltage; the negative reactive power does not mean the resistor produces energy.

Investigation

Compare frequencies below, at and above 2 rad/s for two positive resistances. Retain signed phase, RMS and peak current, real/reactive/apparent power and the power-triangle check. Explain why cancellation of net reactance does not imply zero instantaneous energy in L and C.

Changed-case practice

Try the changed case before feedback

At resonance with R=3 Ω and the same 6 V RMS source, find RMS current in amperes.

This practice is public and unsaved. A matching number does not verify understanding. Retain your explanation, assumptions and changed-case evidence in the separate course workspace.

Sources and boundaries

Original derivations and synthetic evidence checked 31 October 2026 against the primary explanation. Constants are rounded teaching values and are mutually consistent where Maxwell relations require it. No live circuit, high-voltage, energized-inductor, magnet, beam or optical exposure activity is requested. Retain first work, criterion-linked critique, revision and newly assigned evidence; public numerical feedback is not practical or learner certification.

Apply

At omega=2 rad/s and R=2 Ω, what is average real power?

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Which source, initial-state, calibration or field-law premise makes the result conditional, and what unused evidence would challenge it?

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