Why Does a Resistor Show Different Values in AC and DC Measurements?

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SUMMARY

The resistance of a resistor can exhibit different values when measured with alternating current (AC) versus direct current (DC) due to several factors. Key reasons include the skin effect, where current flows primarily on the surface of the conductor, and the presence of inductive and capacitive behaviors in AC circuits. When measuring AC, the root mean square (RMS) values of voltage and current are used, leading to different resistance calculations compared to DC measurements. Understanding these principles is essential for accurate circuit analysis and design.

PREREQUISITES
  • Understanding of Ohm's Law and its application in AC and DC circuits
  • Familiarity with the concepts of root mean square (RMS) values
  • Knowledge of skin effect and its impact on resistance in AC circuits
  • Basic principles of inductance and capacitance in electrical components
NEXT STEPS
  • Study the impact of skin effect on resistors in high-frequency AC applications
  • Learn about the calculation and significance of RMS values in AC circuit analysis
  • Explore the role of inductance and capacitance in AC circuits and their effects on overall resistance
  • Investigate practical examples of measuring resistance in both AC and DC circuits
USEFUL FOR

Electrical engineers, physics students, and anyone involved in circuit design or analysis will benefit from this discussion, particularly those focusing on the differences between AC and DC measurements in resistive components.

The_Lobster
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Homework Statement


If possible, find reasons why the resistance of a resistor may have a different value when measured with a sine wave signal (a.c.) than when measured with a d.c. (dirrect current) source.


Homework Equations




The Attempt at a Solution


Please correct me if anything of what I've said below could be wrong in some way:

In an AC circuit, the sinusoidal current through a resistor is given by: i = Isin \omega t. From Ohm's law, the instantaneous potential v_R is: v_R = iR = (IR)sin \omega t = V_R sin \omega t.

What I don't get here, is that, according to the equation v_R = iR, the relationship between the instantaneous voltage and current is constant (giving R), but if we graph this, since the two are in phase, both the current and the voltage across the resistor will be 0 once every cycle. Doesn't that mean that the resistance, R, of the resistor will also vary? In this illustration: http://www.electronics-tutorials.ws/resistor/res32.gif , we also see that the voltage has steeper curves than the current, and they're not proportional, so v_R = iR isn't true? I find this really confusing...

If we only look at the peak voltages, the resistance would be the peak of the voltage divided by the peak of the current.. it's only when we're talking about instantaneous current and voltage I'm getting confused...

Aside from what I've written above, whenever the frequency of the changing current in a circuit is any other than 0 (DC), any circuit element will exhibit some combination of resistive, capacitive and inductive behaviour. May this mean that we might see a slight drop in resistance measured on the resistor because of the "imagined" inductor in series with it?

Lastly, I read about something called the "skin effect" and the proximity effect that might effect circuit elements when there's an alternating current. Is this something different than the above? Or is it simply another way of saying that each element exhibits some inductive, capaticive, etc. behaviour?

J:-)
 
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The_Lobster said:

Homework Statement


If possible, find reasons why the resistance of a resistor may have a different value when measured with a sine wave signal (a.c.) than when measured with a d.c. (dirrect current) source.


Homework Equations




The Attempt at a Solution


Please correct me if anything of what I've said below could be wrong in some way:

In an AC circuit, the sinusoidal current through a resistor is given by: i = Isin \omega t. From Ohm's law, the instantaneous potential v_R is: v_R = iR = (IR)sin \omega t = V_R sin \omega t.

What I don't get here, is that, according to the equation v_R = iR, the relationship between the instantaneous voltage and current is constant (giving R), but if we graph this, since the two are in phase, both the current and the voltage across the resistor will be 0 once every cycle. Doesn't that mean that the resistance, R, of the resistor will also vary? In this illustration: http://www.electronics-tutorials.ws/resistor/res32.gif , we also see that the voltage has steeper curves than the current, and they're not proportional, so v_R = iR isn't true? I find this really confusing...

If we only look at the peak voltages, the resistance would be the peak of the voltage divided by the peak of the current.. it's only when we're talking about instantaneous current and voltage I'm getting confused...

Aside from what I've written above, whenever the frequency of the changing current in a circuit is any other than 0 (DC), any circuit element will exhibit some combination of resistive, capacitive and inductive behaviour. May this mean that we might see a slight drop in resistance measured on the resistor because of the "imagined" inductor in series with it?

Lastly, I read about something called the "skin effect" and the proximity effect that might effect circuit elements when there's an alternating current. Is this something different than the above? Or is it simply another way of saying that each element exhibits some inductive, capaticive, etc. behaviour?

J:-)

When measuring AC quantities you use rms. So the resistance is the ratio of the rms of the voltage and the rms value of the current.
The reasons to measure different values in AC and DC are the other ones you cited: skin effect (most resistors are made of a thin layer of conductive material over a ceramic substrate), inductance and capacitance.
 

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