4.4.22 · Maths › Multivariable Calculus
Ek double (ya triple) integral bas "chote-chote pieces ko add karo" hai. Kisi flat plate ya solid body ki har physical quantity ek hi recipe se banti hai:
Total quantity = ∬ R ( quantity per tiny piece ) d A
Mass, centre of mass, aur moment of inertia mein sirf yahi change hota hai ki tiny piece of mass ko add karne se pehle usme kya multiply karte hain :
1 se multiply karo → mass .
axis se distance se multiply karo → moment (pehli power) → centre of mass.
axis se distance² se multiply karo → moment of inertia (doosri power).
Ek point mass easy hota hai: uski ek position hoti hai aur ek mass. Lekin ek real plate ka mass ek region R mein density ρ ( x , y ) (mass per unit area) ke saath spread out hota hai. Alag-alag points ki density alag hoti hai aur kisi bhi axis se distance bhi alag hota hai. Isliye hum ek akele number se kaam nahi chala sakte — humein plate ko infinitesimal tiles mein kaatna hoga, har tile ko ek point mass maanna hoga, aur sum (integrate) karna hoga.
Definition Surface density (areal density)
ρ ( x , y ) = point ( x , y ) par mass per unit area . Area d A ki ek tiny tile ka mass hota hai
d m = ρ ( x , y ) d A .
Agar ρ constant ho, toh plate ko homogeneous (uniform) kehte hain.
KYA: total mass = saari tiny masses ka sum.
KAISE (derivation): R ko tiles mein kaato. Tile i ka mass ρ ( x i , y i ) Δ A i hai. Add karo aur refine karo:
m = lim Δ A → 0 ∑ i ρ ( x i , y i ) Δ A i = ∬ R ρ ( x , y ) d A
Intuition "Moment" actually hota kya hai
Ek moment measure karta hai ki kitna mass kitni door ek line se hai — yeh leverage hai. Ek chhota mass door se ek bade mass ko paas mein balance kar sakta hai. Har tile contribute karta hai (uska mass) × (uska lever arm = axis tak ki doori).
Mass se divide KYU karte hain? Centre of mass balance point hota hai — woh akela location jahan tum poora mass rakh sako aur har axis ke baare mein same leverage mile.
Coordinate axes ke baare mein moments define karo. x -axis tak ka lever arm height y hai; y -axis tak ka lever arm x hai.
Centre of mass KAISE milta hai: Balance condition — body ko ( x ˉ , y ˉ ) par ek point mass m se replace karne par same moments milne chahiye:
m x ˉ = M y , m y ˉ = M x .
Solve karo:
Moment of inertia rotation ke against resistance measure karta hai (rotational "mass"). Ek spinning tile ki kinetic energy 2 1 ( d m ) v 2 hoti hai jahan v = ω r , toh energy = 2 1 ω 2 ( r 2 d m ) . r 2 isliye aata hai kyunki speed radius ke saath badhti hai aur energy speed² ke saath badhti hai . r 2 d m ko add karne se rotational inertia milta hai.
Radius of gyration R g = I / m woh akeli distance hai jahan poora mass rakha ho toh same I mile.
Worked example (A) Triangle ka Mass & CoM, variable density
Plate: triangle with vertices ( 0 , 0 ) , ( 1 , 0 ) , ( 0 , 1 ) , density ρ ( x , y ) = x + y .
Mass. Region: 0 ≤ x ≤ 1 , 0 ≤ y ≤ 1 − x .
m = ∫ 0 1 ∫ 0 1 − x ( x + y ) d y d x
Inner pehle KYU? Fixed x ke liye, y bottom edge se slanted line tak jaata hai.
Inner: ∫ 0 1 − x ( x + y ) d y = x ( 1 − x ) + 2 ( 1 − x ) 2 = 2 1 − x 2 .
Yeh step KYU? Bas y mein antiderivative, limits plug karo.
Outer: ∫ 0 1 2 1 − x 2 d x = 2 1 ( 1 − 3 1 ) = 3 1 . Toh m = 3 1 .
M y = ∬ x ρ d A . Inner ∫ 0 1 − x x ( x + y ) d y = x ⋅ 2 1 − x 2 .
Outer ∫ 0 1 2 x − x 3 d x = 2 1 ( 2 1 − 4 1 ) = 8 1 .
Toh x ˉ = m M y = 1/3 1/8 = 8 3 . ρ ki x , y mein symmetry se, y ˉ = 8 3 bhi.
Worked example (B) Uniform rectangle ka Moment of Inertia
Rectangle 0 ≤ x ≤ a , 0 ≤ y ≤ b , constant density ρ .
I x = ρ ∫ 0 a ∫ 0 b y 2 d y d x = ρ ∫ 0 a 3 b 3 d x = 3 ρ a b 3 .
Yeh step KYU? ∫ 0 b y 2 d y = b 3 /3 (andar koi x nahi, isliye outer integral mein constant ki tarah survive karta hai).
Kyunki mass m = ρ ab hai: I x = 3 m b 2 . Similarly I y = 3 m a 2 , aur I 0 = 3 m ( a 2 + b 2 ) .
Worked example (C) Polar ki power — quarter disc
First quadrant mein radius a ka quarter disc, ρ = const. Use karo d A = r d r d θ , x 2 + y 2 = r 2 .
I 0 = ρ ∫ 0 π /2 ∫ 0 a r 2 ⋅ r d r d θ = ρ ⋅ 2 π ⋅ 4 a 4 = 8 π ρ a 4 .
Extra r KYU? Polar coordinates mein ek tile ka area r d r d θ hota hai, na ki d r d θ — ise bhool jaana classic blunder hai (neeche dekho).
Recall Compute karne se pehle predict karo
Radius a ki ek uniform disc ke liye, guess karo : kya I 0 , a 2 ke proportional hai ya a 4 ke?
Forecast: I 0 = ∬ r 2 ρ d A , aur d A (length)² ki tarah scale karta hai. Total scale karega (length)²·(length)² = a 4 ki tarah.
Verify: I 0 = ρ ∫ 0 2 π ∫ 0 a r 3 d r d θ = ρ 2 π 4 a 4 = 2 π ρ a 4 = 2 m a 2 kyunki m = ρ π a 2 . ✓ Wakai ∝ a 4 , aur per-mass ∝ a 2 .
Common mistake "Centre of mass =
x ka average" (ρ bhool jaana)
Kyun sahi lagta hai: uniform plate ke liye density cancel ho jaati hai, toh x ˉ actually geometric average hota hai — centroid. Fix: jab ρ vary kare toh use rakhna zaroori hai: x ˉ = ∬ ρ d A ∬ x ρ d A . Mass position ko weight karta hai.
r d r d θ ki jagah d r d θ use karna
Kyun sahi lagta hai: d x d y ke analogy se lagta hai "bas differentials multiply karo." Fix: ek polar tile ek curved wedge hoti hai jiska area hota hai (radial length)× (arc length)= d r × r d θ . Jacobian factor r mandatory hai.
M x aur I x ko confuse karna
Kyun sahi lagta hai: dono "x-axis ke baare mein hain." Fix: M x mein y 1 use hota hai (balance/CoM ke liye), I x mein y 2 (rotation/energy ke liye). Pehli power vs doosri power.
I 0 = I x + I y hamesha holds karta hai
Kyun sahi lagta hai: yeh ek neat clean formula hai. Fix: yeh perpendicular-axis theorem hai, sirf x y -plane mein planar lamina ke liye valid hai. 3-D solids ke liye yeh fail karta hai.
"1, r , r 2 " — d m ko in se multiply karo:
1 → mass
r (lever arm) → moment → CoM ke liye m se divide karo
r 2 → moment of inertia
Aur polar mein, extra r kabhi mat bhoolo : "polar tiles ek r pehenate hain."
Recall Feynman: ek 12-saal ke bachche ko samjhao
Socho ek pizza jisme cheese kahin moti hai aur kahin patli. Mass hai pizza ki total quantity — tum pizza ke chhote-chhote squares add karte ho. Balance point (centre of mass) woh jagah hai jahan tum pizza ko ek ungli par rakh sako bina girae — yeh heavy side ki taraf jhukta hai, isliye tum har square ko uski doori aur cheese ki moti jagah se weight karte ho. Moment of inertia hai ki pizza ko spin karna kitna mushkil hai: centre se door ki cheese spin ke against zyada ladhti hai nazdeek ki cheese se — aur "door" double-hard count hoti hai kyunki hum distance ko square karte hain. Har baar same recipe: squares mein kaato, har ek ko 1 se, uski distance se, ya uski distance² se multiply karo, phir add karo.
Density aur area ke terms mein d m kya hai? d m = ρ ( x , y ) d A , ek tiny tile ka mass.
Ek lamina ke total mass ka formula? m = ∬ R ρ d A .
Moment M x define karo aur yeh "kis ke baare mein" hai. M x = ∬ R y ρ d A ; x -axis ke baare mein moment (lever arm = y ).
M y define karo.M y = ∬ R x ρ d A (lever arm = x ).
Centre of mass coordinates? x ˉ = M y / m , y ˉ = M x / m .
Centroid aur centre of mass mein kya fark hai? Centroid = CoM jab density constant ho (purely geometric).
x ˉ = M y / m KYU hai (M x / m nahi)?x ˉ y -axis ke baare mein balance karne se aata hai, jiska lever arm x hai, yaani M y .
x -axis ke baare mein moment of inertia?I x = ∬ R y 2 ρ d A .
Origin ke baare mein moment of inertia? I 0 = ∬ R ( x 2 + y 2 ) ρ d A = I x + I y .
I mein distance squared KYU hai?Rotational KE = 2 1 ω 2 ∫ r 2 d m ; speed ∝ r aur energy ∝ v 2 .
Perpendicular axis theorem aur uski limitation? I 0 = I x + I y , sirf flat (planar) lamina ke liye valid hai.
Polar coordinates mein area element? d A = r d r d θ (extra factor r ).
Radius of gyration ki definition? R g = I / m — woh distance jo same
I deti agar poora mass wahan baith jaaye.
Ek uniform rectangle (a × b ) ka I x ? I x = m b 2 /3 = ρ a b 3 /3 .
Radius a ki uniform full disc ka I 0 ? I 0 = 2 1 m a 2 = 2 π ρ a 4 .
Disc ka I 0 radius ke saath kaise scale karta hai? ∝ a 4 (per unit mass ∝ a 2 ).
M x aur I x mein kya fark hai?M x mein y 1 use hota hai (balance); I x mein y 2 (rotation).
treat each tile as point mass
multiply by distance squared
Moment Mx = integral y rho dA
Moment My = integral x rho dA