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.
All lessons are open directly. Your saved experiments remain when you leave and return.
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 experimentPredict
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
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) |
|---|---|
| 0.5 | 0.772988 |
| 0.54375 | 0.8450609 |
| 0.5875 | 0.9181896 |
| 0.63125 | 0.9924285 |
| 0.675 | 1.067822 |
| 0.71875 | 1.1444 |
| 0.7625 | 1.222179 |
| 0.80625 | 1.301156 |
| 0.85 | 1.381307 |
| 0.89375 | 1.462584 |
| 0.9375 | 1.544907 |
| 0.98125 | 1.628167 |
| 1.025 | 1.712214 |
| 1.06875 | 1.796862 |
| 1.1125 | 1.881875 |
| 1.15625 | 1.966973 |
| 1.2 | 2.051823 |
| 1.24375 | 2.136045 |
| 1.2875 | 2.219205 |
| 1.33125 | 2.300824 |
| 1.375 | 2.380384 |
| 1.41875 | 2.45733 |
| 1.4625 | 2.53109 |
| 1.50625 | 2.601083 |
| 1.55 | 2.666738 |
| 1.59375 | 2.727511 |
| 1.6375 | 2.782905 |
| 1.68125 | 2.832487 |
| 1.725 | 2.875905 |
| 1.76875 | 2.9129 |
| 1.8125 | 2.943317 |
| 1.85625 | 2.967106 |
| 1.9 | 2.984324 |
| 1.94375 | 2.995127 |
| 1.9875 | 2.999764 |
| 2.03125 | 2.998559 |
| 2.075 | 2.991898 |
| 2.11875 | 2.980214 |
| 2.1625 | 2.963971 |
| 2.20625 | 2.943646 |
| 2.25 | 2.919719 |
| 2.29375 | 2.89266 |
| 2.3375 | 2.862922 |
| 2.38125 | 2.83093 |
| 2.425 | 2.797081 |
| 2.46875 | 2.761739 |
| 2.5125 | 2.725233 |
| 2.55625 | 2.687858 |
| 2.6 | 2.649875 |
| 2.64375 | 2.611514 |
| 2.6875 | 2.572974 |
| 2.73125 | 2.534427 |
| 2.775 | 2.496021 |
| 2.81875 | 2.45788 |
| 2.8625 | 2.420107 |
| 2.90625 | 2.382789 |
| 2.95 | 2.345997 |
| 2.99375 | 2.309787 |
| 3.0375 | 2.274203 |
| 3.08125 | 2.23928 |
| 3.125 | 2.205044 |
| 3.16875 | 2.171513 |
| 3.2125 | 2.138698 |
| 3.25625 | 2.106606 |
| 3.3 | 2.075238 |
| 3.34375 | 2.044592 |
| 3.3875 | 2.014663 |
| 3.43125 | 1.985442 |
| 3.475 | 1.956921 |
| 3.51875 | 1.929087 |
| 3.5625 | 1.901927 |
| 3.60625 | 1.875428 |
| 3.65 | 1.849574 |
| 3.69375 | 1.82435 |
| 3.7375 | 1.799741 |
| 3.78125 | 1.775731 |
| 3.825 | 1.752303 |
| 3.86875 | 1.729442 |
| 3.9125 | 1.707132 |
| 3.95625 | 1.685356 |
| 4 | 1.664101 |
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.
| Quantity | Value | Unit |
|---|---|---|
| Net reactance | 0 | ohm |
| Impedance magnitude | 2 | ohm |
| RMS current | 3 | A |
| Peak current | 4.242641 | A |
| Voltage-leading-current phase | 0 | rad |
| Average real power | 18 | W |
| Signed reactive power | 0 | var |
| Apparent power | 18 | VA |
| Power factor | 1 | ratio |
| Power-triangle residual | 0 | VA² |
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
Apply
Public practice checks a specific claim. It does not establish independent mastery.
Which source, initial-state, calibration or field-law premise makes the result conditional, and what unused evidence would challenge it?
Continue
Completion requires a saved prediction, at least one capture and a reflection. Presence checks do not grade your reasoning.
Skipping retains experiments and awards no mastery.
Save a science backup or import one
Science work is stored locally in this browser, separately from mathematics and AI. It does not sync automatically. Use this science-only backup; this checkout's older all-subject export does not include science.
A legacy file is available only when the complete snapshot fits the 36 MB limit. For larger snapshots, prepare a complete file set below; never discard notebooks to make a smaller file.
Matching imported notebook drafts replace their current drafts. Omitted lessons and known first attempts remain. Export your current work first if you want to retain both drafts.
Complete file sets and course backups
A file set can hold more work than one science file. Keep its manifest and every part together. Each file is limited to 36 MB. This format needs this version of LearnAI or a compatible newer version; older versions can use only the legacy single-file backup above.
The set includes every saved science course and global continuation at this moment. Later edits need a new export. A conflicting tab exports its own visible work, which may differ from saved work in another tab.
0 file(s) selected. File order and filenames do not determine identity. Missing, changed or conflicting parts block the entire restore; no good part is applied by itself.
Science storage: loading. No account or remote computation is required.