Kitna time laga — usi charge ko zyada time mein cover karna ek weaker flow hai.
Toh natural quantity hai charge divided by time. Shuru karte hain us total charge se jo ek surface cross karta hai:
Q=∫Idt
Agar current steady hai (constant), toh integral collapse ho jaata hai:
Q=I⋅t⟹I=tQ
Yeh step kyun? Integral mein se ek constant ko bahar nikaalte hain toh woh sirf time ki length se multiply hota hai. Yahi everyday form hai jo tum use karte ho.
Changing current ke liye hum limit lete hain, jo instantaneous definition deta hai:
I=limΔt→0ΔtΔQ=dtdQ
Yeh step kyun? Ek choti si window par average ΔQ/Δt wahi exact slope ban jaata hai charge-vs-time curve ka — derivative ka matlab yahi hota hai.
Wire ke andar, current drifting electrons se carry hoti hai. Maano n charge carriers hain per cubic metre, har ek charge q carry karta hai, average speed vd se drift karta hai, ek wire mein jiska cross-sectional area A hai.
Time Δt mein, carriers vdΔt distance move karte hain. AvdΔt volume ke cylinder ke andar saare carriers point se guzar jaate hain:
ΔQ=q⋅n⋅(AvdΔt)
Yeh step kyun? Carriers ki sankhya = density × volume; total charge = woh count × charge-each.
Δt se divide karo:
I=nqAvd
Yeh dikhata hai ki current depend karta hai kitne carriers hain, kitna har ek carry karta hai, wire kitni wide hai, aur kitni tezi se drift karte hain.
Ek busy doorway imagine karo aur tum count karo ki har second kitne log andar se guzarte hain. Electric current bilkul wahi hai, lekin logon ki jagah tiny electric charges hain. "1 ampere" ka matlab hai "1 coulomb-sized bucket of charge har second guzarta hai." Agar har second zyada charge march karta hai, toh current badi hai. Simple hai — bus counting hai!