Griffiths - example 5.5 Electrodynamics - Calculate B Field

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SUMMARY

The forum discussion centers around Example 5.5 from Griffiths' "Introduction to Electrodynamics," specifically the calculation of the magnetic field (B field) at a distance "S" from a current-carrying wire. The user, Sparky, seeks clarification on the transition from the equation tan(θ) = l'/s to dl' = s/cos²(θ) d(θ). The resolution involves recognizing the application of the chain rule in calculus, particularly the derivative of the tangent function, which simplifies the derivation process. This highlights the importance of understanding calculus concepts in electrodynamics problems.

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  • Understanding of calculus, specifically differentiation and the chain rule.
  • Familiarity with Griffiths' "Introduction to Electrodynamics" and its notation.
  • Basic knowledge of magnetic fields and current-carrying wires.
  • Ability to manipulate trigonometric identities and relationships.
NEXT STEPS
  • Review the derivative of the tangent function and its applications in physics.
  • Study the concept of magnetic fields generated by current-carrying conductors.
  • Explore additional examples in Griffiths' text that utilize similar calculus techniques.
  • Practice problems involving the application of the chain rule in physics contexts.
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Students of electromagnetism, physics educators, and anyone seeking to deepen their understanding of calculus applications in electrodynamics.

Sparky_
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Homework Statement



Greetings,

In Griffiths, Introduction to Electrodynamics, example 5.5 (page 216), calculating the B field a distance “S” away from a current carrying wire.

l' (dl’) is the horizontal current carry wire – will be segmented to dl’

tan(\theta) = \frac{l’}{s}

In the next step, it is stated

dl’ = \frac{s}{cos^2(\theta)} d(\theta)

I am stuck on this - I do not see how to get from the first equation to the second. Is there an approximation required?

Homework Equations


The Attempt at a Solution



tan(\theta) = \frac{l’}{s}

and
r^2 = l^2 + s^2

l' = s tan(\theta)

I could square both sides

l^2 = s^2 tan^2(\theta)

l^2 = s^2 \frac{sin^2(\theta)}{cos^2(\theta)}

l^2 = (r^2-l^2) \frac{sin^2(\theta)}{cos^2(\theta)}

\frac{l^2}{(r^2-l^2)} = \frac{sin^2(\theta)}{cos^2(\theta)}

sin^2(\theta) - 1 = \frac{sin^2(\theta)}{cos^2(\theta)}

I do not have this in terms of l' anymore.bottom line how does Griffiths get to

dl’ = \frac{s}{cos^2(\theta)} d(\theta)

from

tan(\theta) = \frac{l’}{s}

Thanks for the help

-Sparky_
 
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Sparky_ said:
tan(\theta) = \frac{l’}{s}

In the next step, it is stated

dl’ = \frac{s}{cos^2(\theta)} d(\theta)

It's easy if you recall the formula for the derivative of the tangent function.
 
  • Like
Likes   Reactions: duarthiago
ah crap - chain rule

I was thinking straight algebra type identity or small angle approximation or some such

did not see the forest for the trees

THANKS!
Sparky_
 

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