Electric Potential and bounds of integration

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SUMMARY

The discussion focuses on calculating the electric potential difference between points V(P) - V(R) and V(c) - V(a) using the integral of the electric field E. The participants highlight confusion regarding the application of the Fundamental Theorem of Calculus, particularly in the evaluation of integral bounds. It is established that the correct evaluation for V(P) - V(R) should yield V(R) - V(P) due to the negative sign in the integral, while V(c) - V(a) aligns with the expected results. The conversation emphasizes the importance of understanding integral bounds in the context of electric potential calculations.

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  • Understanding of electric potential and its mathematical representation.
  • Familiarity with the Fundamental Theorem of Calculus.
  • Knowledge of vector calculus, particularly dot products in integrals.
  • Basic principles of electric fields and work done by electric forces.
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  • Learn about electric field calculations and their relationship to potential differences.
  • Explore vector calculus techniques, particularly in evaluating line integrals.
  • Investigate common pitfalls in calculating electric potential differences in electrostatics.
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timmastny
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Homework Statement



Find the potential difference between V(P) - V(R) and V(c) - V(a)


Homework Equations



Electric potential:

V(a) - V(b) = \int^{b}_{a}E*dr

V(b) - v(a) = -\int^{a}_{b}E*dr

Fundamental Theorem of Calculus:

F(b) - F(a) = \int^{b}_{a}f(x)dx


The Attempt at a Solution



My question is about the solutions attached. In the first example, we have V(P)-V(R), which makes the integral \int^{R}_{P}E*dr. However, when evaluating the integral, the solution takes V(P)-V(R) which seems to disagree with the fundamental theorem of calculus. As per the bounds, I think it should be V(R)-V(P).

Note: while I think it is wrong, the online homework said that evaluting it V(R)-V(P) is incorrect.

Likewise, to add to the confusion, the second picture is the solution for V(c)-V(a), which makes an integral \int^{a}_{c}E*dr. In this case, though, the solution is found by taking v(a)-v(c). (technically v(a) - v(b) because v(c)-v(b) is a constant). This result seems to follow the fundamental theorem of calculus and is the result I expected.

Finally, I thought maybe it had to do with the geometry so I attached a picture of the scenario. Hopefully some one can shed some light on the confusing integral bounds. Thanks
 

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  • Elecpot2.png
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  • electpot.png
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timmastny said:

Homework Statement



Find the potential difference between V(P) - V(R) and V(c) - V(a)


Homework Equations



Electric potential:

V(a) - V(b) = \int^{b}_{a}E*dr
.

No. V(b) - V(a) = -∫E*dr with lower limit of r(a) and upper limit of r(b), with * denoting the vector dot-product. If a unit test charge is moved from a to b where r(a) > r(b) then this integral is positive and represents both the gain in potential and the work done in moving a unit test charge from a to b.

OK, yor formula is not wrong quantitatively but you should think of going from a to b as integrating from a to b, and that means V = -Edr.
 
Last edited:
timmastny said:

Homework Statement



Find the potential difference between V(P) - V(R) and V(c) - V(a)


Homework Equations



Electric potential:

V(a) - V(b) = \int^{b}_{a}E*dr

V(b) - v(a) = -\int^{a}_{b}E*dr

This is a contradiction in terms!
 

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