Returned 96 matches (100 formulae, 58 docs)
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    Found 40064 tuple postings, 23814 formulae, 7117 documents
[ formulas ] [ documents ] [ documents-by-formula ]

1.0000
× 𝐁 = μ 0 𝐉 + μ 0 ϵ 0 t 𝐄 Maxwell s term

0.2847
× 𝐁 = μ 0 𝐉 + μ 0 ϵ 0 𝐄 t

0.2441
× 𝐁 = μ 0 𝐉 + μ 0 ε 0 𝐄 t

0.2403
× 𝐁 = μ 𝐉 + μ ϵ 𝐄 t .

0.2361
× 𝐁 = μ 0 𝐉 + μ 0 ε 0 𝐄 t ,

0.2281
× 𝐁 = μ 0 ϵ 0 𝐄 t ( 4 )

0.2069
× 𝐁 = μ 0 𝐉 + 1 c 2 𝐄 t

0.1942
× 𝐁 = μ 0 𝐉

0.1705
2 𝐁 = μ 0 ϵ 0 2 𝐁 t 2 .

0.1538
× 𝐁 𝟏 = μ 0 𝐉 𝟏 - i ω ϵ 0 μ 0 𝐄 𝟏

0.1508
2 𝐄 = μ 0 ϵ 0 2 𝐄 t 2

0.1456
× 𝐁 = μ 0 𝐣

0.1404
× 𝐁 = μ 0 ε 0 𝐄 t = 1 c 2 𝐄 t

0.1394
× 𝐁 = μ 0 ( 𝐉 + ε 0 𝐄 t )

0.1329
× 𝐁 = 1 c 𝐉 + 1 c 𝐄 t

0.1301
× 𝐁 = 4 π c 𝐉 + 1 c 𝐄 t

0.1283
2 𝐄 - μ 0 ϵ 0 2 𝐄 t 2 = 0.

0.1274
× 𝐁 = 1 ϵ 0 c 2 𝐉 + 1 c 2 𝐄 t

0.1045
× 𝐁 / μ 0 = 𝐉 + ε 0 𝐄 t

0.1035
h t Change in mass over time + h u ¯ x + h v ¯ y Total spatial variation of x,y mass fluxes = 0

0.1022
× 𝐁 = 1 c 𝐄 t + 1 c 𝐉

0.0959
× 𝐇 = 1 c 𝐉 f + 1 c 𝐃 t

0.0943
𝐁 = μ 0 ρ m

0.0940
× ( - 𝐁 t ) = - t ( × 𝐁 ) = - μ 0 ϵ 0 2 𝐄 t 2 ( 7 )

0.0940
× 𝐇 = 4 π c 𝐉 f + 1 c 𝐃 t

0.0935
𝐉 d = ϵ 0 𝐄 t

0.0930
× B = μ 0 J

0.0901
× B = μ 0 J ,

0.0898
× 𝐁 / μ 0 = 𝐉 f + 𝐉 bound + ε 0 𝐄 t

0.0882
× 𝐁 - 1 c 2 𝐄 t = μ 0 𝐉

0.0873
× 𝐁 = 𝐄 t + 𝐉

0.0846
× 𝐁 = 4 π 𝐉 + 𝐄 t

0.0830
2 E - μ 0 ε 0 2 E t 2 = 0.

0.0808
s y m b o l × ( s y m b o l × B ) = μ 0 ϵ 0 t s y m b o l × E .

0.0806
× 𝐇 = 𝐉 f + 𝐃 t

0.0806
1 c 2 2 𝐁 t 2 - 2 𝐁 = μ 0 × 𝐉 .

0.0803
𝐀 = - μ 0 ε 0 φ t

0.0778
× 𝐁 / μ 0 = × ( 𝐇 + 𝐌 )

0.0772
× 𝐁 = 1 c 2 ( 1 ϵ 0 𝐉 + 𝐄 t )

0.0759
𝐤 0 E 0 + ω 0 μ 0 ε 0 E 0 t = 0.

0.0741
× 𝐁 = 1 c ( 4 π 𝐉 + 𝐄 t )

0.0734
2 𝐀 - μ 0 ε 0 2 𝐀 t 2 = 2 𝐀 = - μ 0 𝐉

0.0733
𝐁 = μ 0 ( 𝐇 + 𝐌 ) = 0 ,

0.0732
1 c 2 2 𝐀 t 2 - 2 𝐀 = μ 0 𝐉

0.0726
× 𝐁 = 1 c ( 4 π 𝐉 + 𝐄 t ) .

0.0691
S 𝐁 d 𝐥 = μ 0 S ( 𝐉 + ϵ 0 𝐄 t ) d 𝐀

0.0691
𝐄 = ρ ϵ 0 , × 𝐁 - 1 c 2 𝐄 t = μ 0 𝐉

0.0685
× 𝐇 = 1 c 𝐃 t + 4 π c 𝐉 ,

0.0675
× 𝐇 = 𝐉 + 𝐃 t

0.0661
× 𝐇 = 𝐉 f + 𝐃 t

0.0656
× 𝐇 = 𝐉 + 𝐃 t .

0.0651
× 𝐇 = 4 π c 𝐉 f + 1 c 𝐃 t

0.0643
× 𝐇 = 𝐉 f + t 𝐃 .

0.0643
× 𝐇 = 𝐉 f + 𝐃 t ,

0.0632
× 𝐁 ^ = μ 0 𝐉 ^ + i μ 0 ε 0 ω 𝐄 ^ - B r r + d B ( 1 ) d r + B ( 1 ) r = μ 0 J + i ω μ 0 ε 0 E

0.0625
× 𝐁 = μ 0 𝐣 ; 𝐣 = 2 e m Re { ψ * ( - i - 2 e 𝐀 ) ψ }

0.0619
2 𝐀 - μ 0 ε 0 2 𝐀 t 2 = - μ 0 𝐉 + μ 0 ε 0 ( φ t )

0.0617
× 𝐄 = - 𝐁 t
× 𝐠 = - 𝐇 t

0.0615
𝐁 = μ 0 𝐇

0.0614
E t 0 × 𝐀 = 𝐁 ,

0.0612
× 𝐁 = 0

0.0612
𝐁 = 0 , 𝐁 t + × 𝐄 = 0

0.0603
× 𝐇 = ε o 𝐄 t

0.0603
2 λ - μ 0 ε 0 2 λ t 2 = - 𝐀 - μ 0 ε 0 φ t

0.0603
𝐁 = μ 0 𝐇 ,

0.0601
× 𝐄 = - 𝐁 t ,
× 𝐄 = - 𝐁 t .

0.0599
2 φ - μ 0 ε 0 2 φ t 2 = 2 φ = - ρ ε 0

0.0597
× 𝐁 = α 𝐁

0.0597
s y m b o l τ = 𝐦 × 𝐁 = μ 0 𝐦 × 𝐇 ,

0.0590
2 H z x 2 + 2 H z y 2 = μ ε 2 H z t 2

0.0583
× 𝐄 = - 𝐁 t = 0

0.0583
× 𝐄 = - 𝐁 t ( 2 )

0.0579
𝐃 = ϵ 0 𝐄 , 𝐁 = μ 0 𝐇 .

0.0579
× H = J free + D t

0.0574
× 𝐄 = - 𝐁 t .

0.0571
× E = - B t ,

0.0571
𝐁 = μ 0 ( 𝐇 + 𝐌 )

0.0569
× ( E + A t ) = 0

0.0562
× H = 1 c D t

0.0562
× 𝐄 = - 1 c 𝐁 t

0.0562
× B = 1 c 2 E t .

0.0561
𝐁 = μ 0 ( 𝐇 + 𝐌 ) .

0.0561
𝐒 = 𝐄 × 𝐁 / μ 0

0.0558
r ˙ × H = μ u + c

0.0548
× 𝐁 = 4 π 𝐣 c

0.0547
× 𝐄 = - 1 c 𝐁 t ,

0.0534
( s y m b o l 𝐄 - ρ ϵ 0 ) - c ( s y m b o l × 𝐁 - μ 0 ϵ 0 𝐄 t - μ 0 𝐉 ) + I ( s y m b o l × 𝐄 + 𝐁 t ) + I c ( s y m b o l 𝐁 ) = 0

0.0532
s y m b o l J D = ϵ 0 s y m b o l E t

0.0525
𝐀 + ( 𝐀 + 1 c 2 φ t ) = μ 0 𝐉

0.0520
ρ ( 𝐯 t Unsteady acceleration + ( 𝐯 ) 𝐯 Convective acceleration ) Inertia = - p Pressure gradient + μ 2 𝐯 Viscosity + 𝐟 Other forces

0.0518
s y m b o l × B = μ 0 s y m b o l J D ,
s y m b o l × B = μ 0 s y m b o l J f ,

0.0517
k 0 E 0 z + ω 0 μ 0 ε 0 E 0 t - 1 2 i Δ E 0 = 0.

0.0508
F z ¯ = μ ( z ) F z ,
f z ¯ = μ ( z ) f z ,

0.0504
× ( E + i B ) = i t ( E + i B )

0.0503
× ( α 𝐁 ) = α ( × 𝐁 ) + α × 𝐁 = α 2 𝐁 + α × 𝐁

0.0500
𝐀 = μ 0 𝐉