Magnetostatic Biot–Savart field
A localized steady current distribution in vacuum produces B(r)=μ₀/(4π)∫J(r′)×(r−r′)/|r−r′|³d³r′.
Key knowledge
A localized steady current distribution in vacuum produces B(r)=μ₀/(4π)∫J(r′)×(r−r′)/|r−r′|³d³r′. Charge conservation requires ∇·J=0; in this magnetostatic limit ∇×B=μ₀J and ∇·B=0.
Values and equations
B(r)=μ₀/(4π)∫J(r′)×(r−r′)/|r−r′|³d³r′
- B
- Magnetic flux density T
- J
- Current density A m⁻²
- r,r′
- Positions m
- μ₀
- Vacuum permeability H m⁻¹
Conditions and scope
- Steady divergence-free sources, vacuum and suitable decay/infinity conditions; include the entire closed current circuit.
- Time-varying sources require displacement current and retardation; boundaries and magnetized material require an appropriate additional solution.
Sources · 2
References
Sources retain their recorded scope. A source link alone does not establish verification of every statement.
Richard Fitzpatrick / University of Texas at Austin2 sources
Evidence and review
Classical Electromagnetism (2014): Biot–Savart law: Closed-loop line-current field. Classical Electromagnetism (2014): Continuous current distribution: Equations 616–627: volume-current field and magnetostatic Maxwell laws.
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Entry details
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