Magnetic Field Due to a Curved Wire Segment

In summary, the conversation discussed the use of limits of integration for an integral over the curved path AC. The text did not explicitly state the limits of integration, but the solution could be written as ##\int_S##, where S is the curve AC. The use of a line integral to denote summing the length elements over the path was also mentioned, but this symbol is typically used for integrating around a closed loop.
  • #1
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Homework Statement
Please see below
Relevant Equations
Please see below
For this problem,
1673674584161.png

The solution is,
1673674646262.png

However, why did they not use limits of integration for the integral in red? When I solved this, I used
1673674712595.png

as limits of integration.

I see that is not necessary since you get the same answer either way, but is there a deeper reason?

Many thanks!
 
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  • #2
The text says "integrate over the curved path AC", so it was not essential to write that in the algebra. Also, one does not always have to specify the integration domain as a pair of endpoints. They could have defined S as the curve AC and written ##\int_S##.
 
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  • #3
haruspex said:
The text says "integrate over the curved path AC", so it was not essential to write that in the algebra. Also, one does not always have to specify the integration domain as a pair of endpoints. They could have defined S as the curve AC and written ##\int_S##.
Thanks for your help @haruspex ! That second notation you mention makes more sense than their single integral over ds. I think another way to avoid implicitly defining an integration domain is by using a line integral
1673676771265.png
to denote that we are summing the length elements over the path, correct?
 

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  • #4
Callumnc1 said:
Thanks for your help @haruspex ! That second notation you mention makes more sense than their single integral over ds. I think another way to avoid implicitly defining an integration domain is by using a line integral View attachment 320352to denote that we are summing the length elements over the path, correct?
No, that symbol is for integrating around a closed loop.
 
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  • #5
haruspex said:
No, that symbol is for integrating around a closed loop.
Oh, thank you for your help @haruspex !
 
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FAQ: Magnetic Field Due to a Curved Wire Segment

What is the magnetic field due to a curved wire segment?

The magnetic field due to a curved wire segment can be calculated using the Biot-Savart law, which states that the magnetic field at a point in space is proportional to the current, the length of the wire segment, and the sine of the angle between the wire segment and the point, divided by the square of the distance from the point to the wire segment.

How do you apply the Biot-Savart law to a curved wire segment?

To apply the Biot-Savart law to a curved wire segment, you need to break the wire into infinitesimal segments, calculate the magnetic field contribution from each segment, and then integrate these contributions over the entire length of the curved wire. This often involves setting up an integral in terms of a parameter that describes the curve, such as the angle for a circular arc.

What is the magnetic field at the center of a circular arc of wire?

For a circular arc of wire carrying a current I and subtending an angle θ at the center, the magnetic field at the center of the arc is given by \( B = \frac{\mu_0 I \theta}{4 \pi R} \), where \( \mu_0 \) is the permeability of free space, I is the current, θ is the angle in radians, and R is the radius of the arc.

Does the shape of the wire segment affect the magnetic field it produces?

Yes, the shape of the wire segment significantly affects the magnetic field it produces. The magnetic field depends on the geometry of the wire, including its curvature and the position of the point where the field is being calculated. Different shapes will result in different magnetic field distributions.

How do you calculate the direction of the magnetic field due to a curved wire segment?

The direction of the magnetic field due to a curved wire segment can be determined using the right-hand rule. Point the thumb of your right hand in the direction of the current, and curl your fingers around the wire. Your fingers will point in the direction of the magnetic field lines. For a curved segment, this rule applies locally at each infinitesimal segment of the wire.

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