Ise ek plain number ("scalar") jaise temperature se compare karo — usme sirf size hoti hai, koi direction nahi. Magnetic field directional hai (har jagah kisi direction mein point karti hai), isliye hume arrows ki zaroorat hai ise describe karne ke liye.
Figure s01. Ek single vector: yeh ek point se start hota hai (black dot), iski length iski size hai, aur iski arrowhead (orange) iski direction hai. Dotted plum lines dikhate hain ki usi arrow ko ek horizontal part aur ek vertical part mein split kiya ja sakta hai — ek trick jo hum baad mein dot product ke liye reuse karte hain.
Picture: ek arrow jo ek point se start hokar kahin point karta hai.
Topic ko kyun chahiye: magnetic field B ek vector hai — space ke har point par iske paas ek strength aur ek direction hai. "Field ka path ke saath push" ke baare mein baat karna bina arrows ke possible nahi.
Picture:I = ek pipe mein total flow; J = pipe ke munh par har jagah flow kitna dense hai; dA = us munh se bahar nikalta arrow, aur hum sirf us flow ko count karte hain jo iske saath ja raha hai.
Topic ko kyun chahiye:B ka source current hai. Parent ke Worked Example 2 (radius R ki thick wire, dekho §8) ko J=I/(πR2) chahiye yeh jaanne ke liye ki ek chhote circle ke andar kitni current hai.
Bade integral se pehle hume samajhna hai ki field ka "tumhe path ke saath push karna" matlab kya hai. Woh word along hi dot product hai.
Figure s02. Step dl (orange) path ke saath lie karta hai. Field B (teal) angle θ par lean kar raha hai. B ko step direction par seedha giraao (dotted plum) aur thick plum segment along-path part hai, ∣B∣cosθ. Woh length, step length se multiply hokar, B⋅dl hai.
Saare cases jo tumhe yaad rakhne chahiye:
θ=0∘: cosθ=1 → poora push. (Wire loop mein use hota hai: B circle ke saath run karta hai.)
θ=90∘: cosθ=0 → zero. (Solenoid mein use hota hai: rectangle ke chhote sides B ke perpendicular hote hain.)
Topic ko kyun chahiye:B⋅dl ki har appearance "field-along-path" hai. Clever loops choose karne ka poora method θ ko ya toh 0 (constant push) ya 90∘ (zero) banana hai.
Picture: ek curve hazaron tiny arrows mein toot jaata hai ek dusre ke saath nose-to-tail; har ek dl hai.
Topic ko kyun chahiye: "path ke saath push add karne" ke liye hum path ko tiny steps dl mein chop karte hain, har ek ka along-part B⋅dl lete hain, aur unhe sum karte hain.
Figure s03. Teal circle page se bahar point karne wale wire ke aas-paas Amperian loop C hai. Orange arrows steps dl hain; yahan hum counter-clockwise chalte hain. B field same direction mein wrap karta hai, isliye har B⋅dl poora positive push hai, aur unka total circulation hai. Plum arrow perpendicular distance s mark karta hai.
Topic ko kyun chahiye: Ampère's law ka poora left-hand side yahi circulation hai. Magical claim yeh hai ki yeh total simple hai chahe har step complicated ho.
Ampère's law do cheezein compare karta hai — woh direction jis taraf tum C ke around chalte ho, aur woh direction jis taraf current surface se guzarne par positive count hoti hai. Inhe ek fixed convention se tie karna zaroori hai, warna signs bigad jaate hain.
Picture: fingers counter-clockwise curl kar rahe hain (jaise Figure s03 mein) → thumb page se bahar point karta hai → page se bahar flow karne wali current positive hai.
Topic ko kyun chahiye: iske bina usi wire ko encircle karne wala loop +μ0I ya −μ0I de sakta hai. Rule ambiguity hata deta hai, aur yahi right-hand rule hai jo batata hai B wire ke aas-paas kis taraf wrap karta hai (§9).
Topic ko kyun chahiye: har geometric answer (wire, thick wire, solenoid, toroid) in circle facts ko loop length ya pierced area compute karne ke liye use karta hai. s (distance out) aur R (wire radius) ko alag names rakhna thick-wire case mein zaroori hai jahan J=I/(πR2) hai lekin tum chhote radius s<R par evaluate karte ho.