How Does the Biot-Savart Law Apply to a Wire Segment with a Circular Arc?

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In summary, the magnetic field at point O for a current-carrying wire segment with two straight portions and a circular arc of radius R can be calculated using the Biot-Savart Law. The equation for the magnetic field is B = (μI/4πR)θ, where θ is the angle subtended by the arc and ds represents the magnitude of the original vector ds. The direction of ds x ȑ is the direction of dB due to the elemental current carrying wire.
  • #1
22990atinesh
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Homework Statement



Calculate the magnetic field at point O for the current-carrying wire segment shown in Figure. The wire consists of two straight portions and a circular arc of radius R, which subtends an angle Ɵ. The arrowheads on the wire indicate the direction of the current(Biot–Savart Law).

Capture.jpg


2. The attempt at a solution

##dB = \frac {μ I}{4π} \frac {ds}{R^2}## - I

##B = \frac {μ I}{4π R^2} \int ds = \frac {μ I}{4π R^2} s = \frac {μ I}{4π R} Θ##

Since s=RΘ

I'm little bit confused in the calcualtion of ds in equation I.
##|\vec {ds} \times \hat r| = |\vec {ds}|.1.sin 90^o = ds##
Does ds here represent the magnitude of the vector perpendicular to the vector ##\vec {ds}## and ##\hat r## or it represents the magnitude of orginal vector ##\vec {ds}##.
 
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  • #2
ds is the magnitude of the vector ds what else could it be?
 
  • #3
dauto said:
ds is the magnitude of the vector ds what else could it be?

I know ds is magnitude of ##\vec{ds}##. My doubt is What does it represents. Does ds here represent the magnitude of the vector perpendicular to the vector ##\vec{ds}## and ##\hat{r}## or it represents the magnitude of orginal vector ##\vec{ds}##.
 
  • #4
ds is the magnitude of the original vector ##\vec{ds}## and the direction of ##\vec {ds} \times \hat r## is the direction of ##d\vec{B}## due to the elemental current carrying wire.
 
  • #5
AGNuke said:
ds is the magnitude of the original vector ##\vec{ds}## and the direction of ##\vec {ds} \times \hat r## is the direction of ##d\vec{B}## due to the elemental current carrying wire.

Thanx I get it :smile:
 

Related to How Does the Biot-Savart Law Apply to a Wire Segment with a Circular Arc?

1. What is the Biot-Savart Law?

The Biot-Savart Law is a fundamental law in electromagnetism that describes the magnetic field created by a current-carrying wire.

2. How is the Biot-Savart Law derived?

The Biot-Savart Law is derived from the principle of superposition, which states that the total magnetic field at a point is the vector sum of the magnetic fields produced by each individual current element in the wire.

3. What is the equation for the Biot-Savart Law?

The equation for the Biot-Savart Law is B = (μ₀/4π) * (I * dl x r)/r³, where B is the magnetic field, μ₀ is the permeability of free space, I is the current, dl is the length of the current element, r is the distance from the current element to the point, and x represents the cross product.

4. What are some applications of the Biot-Savart Law?

The Biot-Savart Law is used in many areas of science and engineering, including electromagnetics, plasma physics, and fluid dynamics. It is also used in practical applications such as designing electromagnets, motors, and generators.

5. Are there any limitations to the Biot-Savart Law?

Yes, the Biot-Savart Law has some limitations. It is only valid for steady currents and does not take into account the effects of changing electric fields. It also assumes an infinitely long, thin current-carrying wire, which may not accurately represent real-life situations.

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