High Pass Filter
About points...
We associate a certain number of points with each exercise.
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.
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 -
Question
Solution
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Exercise:
A simple high pass filter consists of a resistor and an inductor connected in series to the input signal. abcliste abc Show that the partial voltage amplitude across the inductor is given by V_C fracV_sqrtleftfracomega_comegaright^ + where V_ is the amplitude of the input signal and omega_c the cutoff frequency: omega_c sqrtfracRL What is the partial voltage at the cutoff frequency? Sketch the value of V_L/V_ vs frequency. abc For a typical high pass filter used in audio circuits the input signal has an amplitude of VO and the resistance and inductance are RO and LO respectively. Calculate the cutoff frequency and the frequency at which the output voltage i.e. the partial voltage across the inductor is VLO. abcliste
Solution:
abcliste abc The impedance for an RL series circuit is Z sqrtR^+leftomega Lright^ It follows for the partial voltage across the capacitor V_L X_L I_ omega L fracV_Z fracV_ omega LsqrtR^+leftomega Lright^ fracV_sqrtleftfracRomega Lright^+ With fracRL omega_c it follows V_L fracV_leftfracomega_comegaright^+ quad square For omegaomega_c we find V_L fracV_sqrtleftfracomega_comega_cright^+ fracV_sqrt i.e. the voltage across the inductor is sqrt times smaller than the input voltage. vspacemm The diagram below shows how the partial voltage deps on the frequency. center includegraphicswidthtextwidth#image_path:high-pass-filter-# center abc The cutoff angular frequency is omega_c omcF fracRL omc This corresponds to a frequency f_c fracomega_cpi fc approx resultfcP The partial voltage across the inductor is V_L fracV_sqrtleftfracomega_comegaright^+ fracV_sqrtleftfracRpi f Lright^+ Solving for the frequency yields f fF fracRpitimesLtimessqrtleftfracVVLright^- f approx resultfP abcliste
A simple high pass filter consists of a resistor and an inductor connected in series to the input signal. abcliste abc Show that the partial voltage amplitude across the inductor is given by V_C fracV_sqrtleftfracomega_comegaright^ + where V_ is the amplitude of the input signal and omega_c the cutoff frequency: omega_c sqrtfracRL What is the partial voltage at the cutoff frequency? Sketch the value of V_L/V_ vs frequency. abc For a typical high pass filter used in audio circuits the input signal has an amplitude of VO and the resistance and inductance are RO and LO respectively. Calculate the cutoff frequency and the frequency at which the output voltage i.e. the partial voltage across the inductor is VLO. abcliste
Solution:
abcliste abc The impedance for an RL series circuit is Z sqrtR^+leftomega Lright^ It follows for the partial voltage across the capacitor V_L X_L I_ omega L fracV_Z fracV_ omega LsqrtR^+leftomega Lright^ fracV_sqrtleftfracRomega Lright^+ With fracRL omega_c it follows V_L fracV_leftfracomega_comegaright^+ quad square For omegaomega_c we find V_L fracV_sqrtleftfracomega_comega_cright^+ fracV_sqrt i.e. the voltage across the inductor is sqrt times smaller than the input voltage. vspacemm The diagram below shows how the partial voltage deps on the frequency. center includegraphicswidthtextwidth#image_path:high-pass-filter-# center abc The cutoff angular frequency is omega_c omcF fracRL omc This corresponds to a frequency f_c fracomega_cpi fc approx resultfcP The partial voltage across the inductor is V_L fracV_sqrtleftfracomega_comegaright^+ fracV_sqrtleftfracRpi f Lright^+ Solving for the frequency yields f fF fracRpitimesLtimessqrtleftfracVVLright^- f approx resultfP abcliste
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Exercise:
A simple high pass filter consists of a resistor and an inductor connected in series to the input signal. abcliste abc Show that the partial voltage amplitude across the inductor is given by V_C fracV_sqrtleftfracomega_comegaright^ + where V_ is the amplitude of the input signal and omega_c the cutoff frequency: omega_c sqrtfracRL What is the partial voltage at the cutoff frequency? Sketch the value of V_L/V_ vs frequency. abc For a typical high pass filter used in audio circuits the input signal has an amplitude of VO and the resistance and inductance are RO and LO respectively. Calculate the cutoff frequency and the frequency at which the output voltage i.e. the partial voltage across the inductor is VLO. abcliste
Solution:
abcliste abc The impedance for an RL series circuit is Z sqrtR^+leftomega Lright^ It follows for the partial voltage across the capacitor V_L X_L I_ omega L fracV_Z fracV_ omega LsqrtR^+leftomega Lright^ fracV_sqrtleftfracRomega Lright^+ With fracRL omega_c it follows V_L fracV_leftfracomega_comegaright^+ quad square For omegaomega_c we find V_L fracV_sqrtleftfracomega_comega_cright^+ fracV_sqrt i.e. the voltage across the inductor is sqrt times smaller than the input voltage. vspacemm The diagram below shows how the partial voltage deps on the frequency. center includegraphicswidthtextwidth#image_path:high-pass-filter-# center abc The cutoff angular frequency is omega_c omcF fracRL omc This corresponds to a frequency f_c fracomega_cpi fc approx resultfcP The partial voltage across the inductor is V_L fracV_sqrtleftfracomega_comegaright^+ fracV_sqrtleftfracRpi f Lright^+ Solving for the frequency yields f fF fracRpitimesLtimessqrtleftfracVVLright^- f approx resultfP abcliste
A simple high pass filter consists of a resistor and an inductor connected in series to the input signal. abcliste abc Show that the partial voltage amplitude across the inductor is given by V_C fracV_sqrtleftfracomega_comegaright^ + where V_ is the amplitude of the input signal and omega_c the cutoff frequency: omega_c sqrtfracRL What is the partial voltage at the cutoff frequency? Sketch the value of V_L/V_ vs frequency. abc For a typical high pass filter used in audio circuits the input signal has an amplitude of VO and the resistance and inductance are RO and LO respectively. Calculate the cutoff frequency and the frequency at which the output voltage i.e. the partial voltage across the inductor is VLO. abcliste
Solution:
abcliste abc The impedance for an RL series circuit is Z sqrtR^+leftomega Lright^ It follows for the partial voltage across the capacitor V_L X_L I_ omega L fracV_Z fracV_ omega LsqrtR^+leftomega Lright^ fracV_sqrtleftfracRomega Lright^+ With fracRL omega_c it follows V_L fracV_leftfracomega_comegaright^+ quad square For omegaomega_c we find V_L fracV_sqrtleftfracomega_comega_cright^+ fracV_sqrt i.e. the voltage across the inductor is sqrt times smaller than the input voltage. vspacemm The diagram below shows how the partial voltage deps on the frequency. center includegraphicswidthtextwidth#image_path:high-pass-filter-# center abc The cutoff angular frequency is omega_c omcF fracRL omc This corresponds to a frequency f_c fracomega_cpi fc approx resultfcP The partial voltage across the inductor is V_L fracV_sqrtleftfracomega_comegaright^+ fracV_sqrtleftfracRpi f Lright^+ Solving for the frequency yields f fF fracRpitimesLtimessqrtleftfracVVLright^- f approx resultfP abcliste
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