RC series circuit
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But as a guideline, we tend to give as many points by default as there are mathematical steps to do in the exercise.
Again, very vague... But the number should kind of represent the "work" required.
When you click an exercise into a collection, this number will be taken as points for the exercise, kind of "by default".
But once the exercise is on the collection, you can edit the number of points for the exercise in the collection independently, without any effect on "points by default" as represented by the number here.
That being said... How many "default points" should you associate with an exercise upon creation?
As with difficulty, there is no straight forward and generally accepted way.
But as a guideline, we tend to give as many points by default as there are mathematical steps to do in the exercise.
Again, very vague... But the number should kind of represent the "work" required.
About difficulty...
We associate a certain difficulty with each exercise.
When you click an exercise into a collection, this number will be taken as difficulty for the exercise, kind of "by default".
But once the exercise is on the collection, you can edit its difficulty in the collection independently, without any effect on the "difficulty by default" here.
Why we use chess pieces? Well... we like chess, we like playing around with \(\LaTeX\)-fonts, we wanted symbols that need less space than six stars in a table-column... But in your layouts, you are of course free to indicate the difficulty of the exercise the way you want.
That being said... How "difficult" is an exercise? It depends on many factors, like what was being taught etc.
In physics exercises, we try to follow this pattern:
Level 1 - One formula (one you would find in a reference book) is enough to solve the exercise. Example exercise
Level 2 - Two formulas are needed, it's possible to compute an "in-between" solution, i.e. no algebraic equation needed. Example exercise
Level 3 - "Chain-computations" like on level 2, but 3+ calculations. Still, no equations, i.e. you are not forced to solve it in an algebraic manner. Example exercise
Level 4 - Exercise needs to be solved by algebraic equations, not possible to calculate numerical "in-between" results. Example exercise
Level 5 -
Level 6 -
When you click an exercise into a collection, this number will be taken as difficulty for the exercise, kind of "by default".
But once the exercise is on the collection, you can edit its difficulty in the collection independently, without any effect on the "difficulty by default" here.
Why we use chess pieces? Well... we like chess, we like playing around with \(\LaTeX\)-fonts, we wanted symbols that need less space than six stars in a table-column... But in your layouts, you are of course free to indicate the difficulty of the exercise the way you want.
That being said... How "difficult" is an exercise? It depends on many factors, like what was being taught etc.
In physics exercises, we try to follow this pattern:
Level 1 - One formula (one you would find in a reference book) is enough to solve the exercise. Example exercise
Level 2 - Two formulas are needed, it's possible to compute an "in-between" solution, i.e. no algebraic equation needed. Example exercise
Level 3 - "Chain-computations" like on level 2, but 3+ calculations. Still, no equations, i.e. you are not forced to solve it in an algebraic manner. Example exercise
Level 4 - Exercise needs to be solved by algebraic equations, not possible to calculate numerical "in-between" results. Example exercise
Level 5 -
Level 6 -
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Exercise:
Calculate the impedance and the phase shift for an ac circuit with a resistor resistance RO and a capacitor capacitive reactance XCO in series.
Solution:
Since the resistor and the capacitor are connected in series the same current I flows through both elements; we use it as the reference phasor. The voltage across the resistor V_R RI is in phase with the current while the voltage across the capacitor V_C X_C I lags the current by degree. The total voltage V is the phasor of V_R and V_C. center tikzpicturestealth scale. draw- - -- noderight mathrmRe; draw- - -- nodeabove mathrmIm; draw- blue thick -- nodemidway above I; draw- red thick -- nodemidway below V_R; draw- red thick -- - nodemidway right V_C; draw- red ultra thick -- - nodemidway below left V; draw arc :-.:; node at - varphi; tikzpicture center Dividing every phasor in the diagram by the real in-phase current I turns the voltage triangle o the impedance triangle since ZV/I RV_R/I and X_CV_C/I. From this right triangle we read off the magnitude of the total impedance and the phase angle varphi between the total voltage V and the current I: Z fracVI sqrtR^+X_C^ sqrtR^+XC^ Z approx resultZP varphi -arctanleftfracV_CV_Rright -arctanleftfracX_CRright -arctanleftfracXCRright ph approx resultphP medskip Alternatively we can assign a complex quantity to each element. The resistor's contribution is purely real R while the capacitor's complex reactance is tilde X_C -iX_C since the current through a capacitor leads the voltage across it by degree. As the elements are in series the complex impedances add: tilde Z R + tilde X_C R - iX_C The magnitude and the argument of this complex number reproduce exactly the impedance and phase shift found above: Z |tilde Z| sqrtR^+X_C^ Z approx resultZP varphi argtilde Z -arctanleftfracX_CRright ph approx resultphP confirming the result obtained with the phasor diagram.
Calculate the impedance and the phase shift for an ac circuit with a resistor resistance RO and a capacitor capacitive reactance XCO in series.
Solution:
Since the resistor and the capacitor are connected in series the same current I flows through both elements; we use it as the reference phasor. The voltage across the resistor V_R RI is in phase with the current while the voltage across the capacitor V_C X_C I lags the current by degree. The total voltage V is the phasor of V_R and V_C. center tikzpicturestealth scale. draw- - -- noderight mathrmRe; draw- - -- nodeabove mathrmIm; draw- blue thick -- nodemidway above I; draw- red thick -- nodemidway below V_R; draw- red thick -- - nodemidway right V_C; draw- red ultra thick -- - nodemidway below left V; draw arc :-.:; node at - varphi; tikzpicture center Dividing every phasor in the diagram by the real in-phase current I turns the voltage triangle o the impedance triangle since ZV/I RV_R/I and X_CV_C/I. From this right triangle we read off the magnitude of the total impedance and the phase angle varphi between the total voltage V and the current I: Z fracVI sqrtR^+X_C^ sqrtR^+XC^ Z approx resultZP varphi -arctanleftfracV_CV_Rright -arctanleftfracX_CRright -arctanleftfracXCRright ph approx resultphP medskip Alternatively we can assign a complex quantity to each element. The resistor's contribution is purely real R while the capacitor's complex reactance is tilde X_C -iX_C since the current through a capacitor leads the voltage across it by degree. As the elements are in series the complex impedances add: tilde Z R + tilde X_C R - iX_C The magnitude and the argument of this complex number reproduce exactly the impedance and phase shift found above: Z |tilde Z| sqrtR^+X_C^ Z approx resultZP varphi argtilde Z -arctanleftfracX_CRright ph approx resultphP confirming the result obtained with the phasor diagram.
Meta Information
Exercise:
Calculate the impedance and the phase shift for an ac circuit with a resistor resistance RO and a capacitor capacitive reactance XCO in series.
Solution:
Since the resistor and the capacitor are connected in series the same current I flows through both elements; we use it as the reference phasor. The voltage across the resistor V_R RI is in phase with the current while the voltage across the capacitor V_C X_C I lags the current by degree. The total voltage V is the phasor of V_R and V_C. center tikzpicturestealth scale. draw- - -- noderight mathrmRe; draw- - -- nodeabove mathrmIm; draw- blue thick -- nodemidway above I; draw- red thick -- nodemidway below V_R; draw- red thick -- - nodemidway right V_C; draw- red ultra thick -- - nodemidway below left V; draw arc :-.:; node at - varphi; tikzpicture center Dividing every phasor in the diagram by the real in-phase current I turns the voltage triangle o the impedance triangle since ZV/I RV_R/I and X_CV_C/I. From this right triangle we read off the magnitude of the total impedance and the phase angle varphi between the total voltage V and the current I: Z fracVI sqrtR^+X_C^ sqrtR^+XC^ Z approx resultZP varphi -arctanleftfracV_CV_Rright -arctanleftfracX_CRright -arctanleftfracXCRright ph approx resultphP medskip Alternatively we can assign a complex quantity to each element. The resistor's contribution is purely real R while the capacitor's complex reactance is tilde X_C -iX_C since the current through a capacitor leads the voltage across it by degree. As the elements are in series the complex impedances add: tilde Z R + tilde X_C R - iX_C The magnitude and the argument of this complex number reproduce exactly the impedance and phase shift found above: Z |tilde Z| sqrtR^+X_C^ Z approx resultZP varphi argtilde Z -arctanleftfracX_CRright ph approx resultphP confirming the result obtained with the phasor diagram.
Calculate the impedance and the phase shift for an ac circuit with a resistor resistance RO and a capacitor capacitive reactance XCO in series.
Solution:
Since the resistor and the capacitor are connected in series the same current I flows through both elements; we use it as the reference phasor. The voltage across the resistor V_R RI is in phase with the current while the voltage across the capacitor V_C X_C I lags the current by degree. The total voltage V is the phasor of V_R and V_C. center tikzpicturestealth scale. draw- - -- noderight mathrmRe; draw- - -- nodeabove mathrmIm; draw- blue thick -- nodemidway above I; draw- red thick -- nodemidway below V_R; draw- red thick -- - nodemidway right V_C; draw- red ultra thick -- - nodemidway below left V; draw arc :-.:; node at - varphi; tikzpicture center Dividing every phasor in the diagram by the real in-phase current I turns the voltage triangle o the impedance triangle since ZV/I RV_R/I and X_CV_C/I. From this right triangle we read off the magnitude of the total impedance and the phase angle varphi between the total voltage V and the current I: Z fracVI sqrtR^+X_C^ sqrtR^+XC^ Z approx resultZP varphi -arctanleftfracV_CV_Rright -arctanleftfracX_CRright -arctanleftfracXCRright ph approx resultphP medskip Alternatively we can assign a complex quantity to each element. The resistor's contribution is purely real R while the capacitor's complex reactance is tilde X_C -iX_C since the current through a capacitor leads the voltage across it by degree. As the elements are in series the complex impedances add: tilde Z R + tilde X_C R - iX_C The magnitude and the argument of this complex number reproduce exactly the impedance and phase shift found above: Z |tilde Z| sqrtR^+X_C^ Z approx resultZP varphi argtilde Z -arctanleftfracX_CRright ph approx resultphP confirming the result obtained with the phasor diagram.
Contained in these collections
| Title | Matched on |
|---|---|
| RL parallel circuit | formula |
| RC Series Circuit | title |
| Partial Voltages in RC Circuit | formula |
| LCR Series Circuit | title |
| Partial Currents in Parallel Circuit | formula |

