Match the following Maxwell's equations with their names in the case of static fields. Gauss's law in electrostatics (A) VxB=HJ (B) V-B-0 (C) VxE=0 (11) (11) (iv) Gauss's law in magnetostatics Faraday's law Amper's law (D) V.E= -B (E) VxE== at (F)√x B= μJ+μs! (i) → (D), (ii) → (B), (iii) → (C), (iv) → (A) (b) (i) → (D), (ii) → (c) ) → (C), (ii) ➜ (d) (i) → (D), (ii) → (B), (iii) → (E), (iv) → (C) (E), (in) → (D), (iv) → (F) (B), (iii) → (E), (iv) → (F) aE at
Match the following Maxwell's equations with their names in the case of static fields. Gauss's law in electrostatics (A) VxB=HJ (B) V-B-0 (C) VxE=0 (11) (11) (iv) Gauss's law in magnetostatics Faraday's law Amper's law (D) V.E= -B (E) VxE== at (F)√x B= μJ+μs! (i) → (D), (ii) → (B), (iii) → (C), (iv) → (A) (b) (i) → (D), (ii) → (c) ) → (C), (ii) ➜ (d) (i) → (D), (ii) → (B), (iii) → (E), (iv) → (C) (E), (in) → (D), (iv) → (F) (B), (iii) → (E), (iv) → (F) aE at
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Transcribed Image Text:Match the following Maxwell's equations with their names in the case of static fields.
(1)
Gauss's law in electrostatics
(A) V x B= UJ
(11)
Gauss's law in magnetostatics
(B) V-B=0
(111)
Faraday's law
(C) VxE=0
(iv)
Amper's law
(D) V.E=
(E) VxE=
(F) ▼x B= μJ+ µE !
(a) (i) → (D), (ii) → (B), (iii) → (C), (iv) → (A)
(b) (i) → (D), (ii) → (B), (iii) → (E), (iv) → (C)
(c) (i) → (C), (11) ➜ (E), (iii) → (D), (iv) → (F)
(d) (i) → (D), (ii) → (B), (iii) ➜ (E), (iv) → (F)
-aB
at
aE
at
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