Voltage drop: What do we mean when we say that voltage drops across a resistor?

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SUMMARY

The discussion centers on the concept of voltage drop across a resistor, emphasizing that one end of the resistor is at a lower electrostatic potential than the other. This voltage drop is a manifestation of Kirchhoff's Voltage Law (KVL), which states that the total potential difference in a closed circuit is zero. The conversation also clarifies that while a battery creates a potential difference, electrons do not pass through the battery; instead, a chemical reaction separates charges, leading to the voltage measured across its terminals. The unit of voltage is defined as one volt, equivalent to one joule per coulomb.

PREREQUISITES
  • Understanding of Kirchhoff's Voltage Law (KVL)
  • Basic knowledge of electric potential and voltage
  • Familiarity with the concept of electromotive force (emf)
  • Awareness of Ohm's Law and its applications
NEXT STEPS
  • Research the principles of Kirchhoff's Voltage Law (KVL) in detail
  • Study the chemical processes in batteries and their role in creating potential differences
  • Explore the relationship between electric potential and potential energy per unit charge
  • Learn about the implications of electron theory in circuit analysis and its limitations
USEFUL FOR

Electrical engineering students, circuit designers, educators in physics, and anyone seeking to deepen their understanding of voltage, resistors, and circuit theory.

Bheshaj
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What do we mean when we say that voltage drops across a resistor?and what does it mean when we say that a point is at lower potential as compared to some other point?Can we say that potential is potential energy per unit charge?
 
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Bheshaj said:
What do we mean when we say that voltage drops across a resistor?
We mean that the voltage is lower at one end of the resistor than it is at the other end.
and what does it mean when we say that a point is at lower potential as compared to some other point?
We mean that one point has a lower voltage than another point.
 
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To add to @phinds's response
We mean that one end of the resistor is at a lower electrostatic potential than the other. Note that the convention in circuits is that straight lines are considered equipotentials. Here is a gravitational analogy to help you picture it. A straight line in a circuit is like walking a horizontal corridor - no change in gravitational potential energy. Stairs are like resistors. If you encounter stairs going up, you have a rise in gravitational potential from the bottom of the stairs to the top. If you encounter stairs going down, you have a drop in gravitational potential from the top of the stairs to the bottom. The same idea applies to electric potential. BTW, if you walk inside a building and visit various people on various floors but eventually end up where you started, the sum of all your potential rises and drops is zero. The same applies to charge carriers in electric circuits and the idea is called Kirchhoff's Voltage Law (KVL).
 
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kuruman said:
To add to @phinds's response
We mean that one end of the resistor is at a lower electrostatic potential than the other. Note that the convention in circuits is that straight lines are considered equipotentials. Here is a gravitational analogy to help you picture it. A straight line in a circuit is like walking a horizontal corridor - no change in gravitational potential energy. Stairs are like resistors. If you encounter stairs going up, you have a rise in gravitational potential from the bottom of the stairs to the top. If you encounter stairs going down, you have a drop in gravitational potential from the top of the stairs to the bottom. The same idea applies to electric potential. BTW, if you walk inside a building and visit various people on various floors but eventually end up where you started, the sum of all your potential rises and drops is zero. The same applies to charge carriers in electric circuits and the idea is called Kirchhoff's Voltage Law (KVL).
Thanks now I am able to interpret. Can we say that after battery creates a potential diiference, electron gains potential energy as it passes through it and the difference in potential energy per unit charge between two pointsis called voltage between the two points. Am I right?
 
Bheshaj said:
Thanks now I am able to interpret. Can we say that after battery creates a potential diiference, electron gains potential energy as it passes through it and the difference in potential energy per unit charge between two pointsis called voltage between the two points. Am I right?
Recall that the unit of voltage is the volt, which is equal to one joule per coulomb. So if you have a one volt battery, an electron passing through it will gain potential energy equal to the voltage of the battery times the charge of the particle. So yes, the particles passing through batteries will gain potential energy, but the magnitude of this energy gain is dependent on the charge of the particle.
 
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I'd say, a battery provides and electromotive force (emf) rather than a voltage in the strict sense. The word "force" is a bit unfortunate and must be read in the historical context. In the early 19th century, when the energy concept came up, famously mostly due to Helmholtz's discovery of what we call "energy conservation law" today, the word "force" meant in fact "energy". Helmholtz's famous paper is titled "Über die Erhaltung der Kraft" ("On the conservation of force"), but here "force" in fact means what we call "energy" today. Wikipedia gives a pretty good definition of the emf in its various forms

https://en.wikipedia.org/wiki/Electromotive_force
 
Bheshaj said:
Can we say that after battery creates a potential difference, the electron gains potential energy as it passes through it

No
An electron (electrons) don't pass through the battery. Very simply, a battery uses a chemical reaction
to separate charges. Negative charges ( electrons) move onto one terminal and positive charges ( ions)
onto the other terminal. This is what causes the potential difference ( the voltage measured on a voltmeter)
between the two terminals.
 
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vanhees71 said:
For a very nice pedgagogical paper, see

https://doi.org/10.1119/1.13128
unfortunately that's a limited access site. would have been interesting to read :smile:
 
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I am a bit confused whether electron passes through a battery or no. My book says battery pumps electrons so it should be the case am I right?
 
  • #11
Can we say that potential difference is potential energy difference per unit charge. when positive charges move from higher potential to lower potential does their potential energy decrease . And when they they pass through battery does the potential energy per unit charge decrease.Can we conclude that potential at a point gives the potential energy per unit charge at that point or am I wrong please clarify
 
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Bheshaj said:
I am a bit confused whether electron passes through a battery or no. My book says battery pumps electrons so it should be the case am I right?
Forget you ever heard the word "electron". They are irrelevant to circuit theory.

In any case, no single electron needs to make a complete round trip through circuit and battery in order for current to flow.
 
  • #13
jbriggs444 said:
Forget you ever heard the word "electron". They are irrelevant to circuit theory.
:bow: amen
 
  • #14
Hm, this is a bit problematic to say. To understand the constitutive laws, even in a schematic classical way, the idea of electrons are important.

E.g., often Ohm's law is stated as
$$\vec{j}=\sigma \vec{E},$$
without the qualification that this is valid in the non-relativistic limit only. Of course it's valid for usual household currents in usual household cables. How do you explain this, if not using electrons (though in the classical sense)?

The complete law (in Heaviside Lorentz units) must be
$$\vec{j}=\sigma(\vec{E}+\vec{v}/c \times \vec{B}).$$
This becomes important in the theory of the homopolar generator, which looks only "non-relativistic" on a superficial view. In this case the neglegence of relativity and (at least) classical electron theory leads to misconceptions and paradoxes!

Abandon the "fluid analogy" rather than the "classical-electron theory" as heuristics in circuit theory!
 
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