1.2.16 · D1 · Physics › Newton's Laws & Dynamics › Centripetal force — what provides it in various situations
Jo bhi circle mein move kar raha hai woh turn kar raha hai, aur turn karne ka matlab hai ki uski direction of motion continuously change ho rahi hai — woh change hi ek acceleration hai jo hamesha middle ki taraf point karti hai. Us turn ko make karne ke liye, koi real force (ek string, gravity, friction, ek magnet…) zaroor woh inward pull supply karni chahiye; "centripetal force" bas ek job-title hai jo hum us real force ko dete hain jo woh pulling kar rahi hai. (Hum neeche har symbol build karte hain pehle koi bhi formula likhne se.)
Pehle tum parent note Centripetal force — what provides it padh sako, tumhare paas har woh symbol hona chahiye jo woh tumhare saamne phenkta hai. Hum unhe ek-ek karke build karte hain, har ek us picture se jo uske saath rehti hai.
Definition Moving body ko ek
point maano
Hum poore object (patthar, car, planet) ko ek single point mein shrink kar dete hain jo ek path trace karta hai. Hum jo bhi bolte hain woh is baare mein hai ki woh point kahan hai aur woh kitni tez move karta hai .
Ek dot ko ek curved track par slide karte hue imagine karo. Woh dot hi abhi ke liye hamaari poori duniya hai.
r — radius
r (seedhe alfazon mein: "point middle se kitni door baitha hai") center se moving point tak ki fixed distance hai. Uski picture: ek wheel ke hub se rim tak ek seedha spoke.
Figure dekho: orange dot moving point hai, magenta spoke r hai, aur black cross center hai. Kyunki point circle par rehta hai, yeh spoke kabhi apni length nahi badlata — yahi constancy isse ek circle banati hai na ki koi wobbly loop. Is topic ko r ki zaroorat hai kyunki, jaise hum dekhenge, required inward pull kamzor hoti jaati hai jab circle wider hoti jaati hai (bada r ).
Intuition Arrow kyun, sirf number kyun nahi?
Speed jaise "5 m/s" sirf ek size hai. Lekin kis taraf point move karta hai yeh utna hi matter karta hai. Ek arrow — ek vector — dono store karta hai size (uski length) aur direction (jahan woh point karta hai). Hum vectors ke upar ek chhota arrow likhte hain: v .
v — velocity vector
v (seedhe alfazon mein: "point abhi kitni tez aur kis direction mein move kar raha hai"). Uski picture: ek chhota arrow point se chipka hua, track ke along point karta hua — woh direction jisme woh iss instant release hone par fly off kar jaata.
Figure dekho: circle par har jagah violet velocity arrow tangent lie karta hai — woh circle ko bas graze karta hai, hamesha magenta spoke r ke right angle (9 0 ∘ ) par. Yeh right-angle fact derivation mein baar baar use hota hai, toh ise abhi se lock kar lo.
∣ v ∣ aur v — speed
Do vertical bars ka matlab hai "length of." ∣ v ∣ velocity arrow ki length hai = plain speed, jise simply v likhte hain (koi arrow nahi). Picture: arrow ko ruler se measure karo; woh number v hai.
Δ — "mein change"
Δ (Greek capital delta ) kisi bhi cheez ke aage matlab hai "final minus initial" — yeh kitna badla. Toh Δ t time ka ek chhota hissa hai, aur Δ v = v final − v initial hai ki velocity arrow kaise badla.
Intuition Do arrows subtract karna — picture
v 2 − v 1 arrows se karne ke liye: dono tails ko ek hi jagah rakho; woh arrow jo v 1 ki tip se v 2 ki tip tak jaata hai woh difference Δ v hai. Chahe v 1 aur v 2 ki length same ho (same speed), agar woh alag taraf point karte hain toh yeh connecting arrow zero nahi hoga.
Figure dekho: do violet arrows length mein equal hain (speed unchanged) lekin ek chhote angle se rotated apart hain. Orange arrow jo unki tips ko bridge karta hai woh Δ v hai — aur notice karo ki woh roughly original circle ke center ki taraf point karta hai. Yahi centripetal acceleration ka beej hai: constant speed par bhi velocity mein non-zero change.
a — acceleration
a (seedhe alfazon mein: "velocity khud kitni tez change ho rahi hai") Δ t Δ v hai — change-in-velocity arrow divided by woh chhota time jo laga. Picture: upar se orange Δ v arrow lo aur use ek chhote number Δ t se divide karke stretch/shrink karo; yeh direction same rakhta hai (center ki taraf) lekin rescale ho jaata hai.
Kyunki Δ v inward point karta tha, a bhi inward point karta hai. Yahi centripetal ("center-seeking") acceleration hai.
θ — ek angle
θ (Greek theta , seedhe alfazon mein: "kitna around, ya kitna tilted") rotation ya tilt measure karta hai. Δ θ time Δ t ke dauran center ke around point ka chhota turn hai.
radians mein measure kyun karein
Ek radian aise define hota hai ki arc length = radius × angle . Picture: length r ki ek string ka ek tukda rim ke along bend karo; center par jo angle subtend hota hai woh exactly 1 radian hota hai. Hum radians choose karte hain (degrees nahi) precisely kyunki woh "arc = r θ " ko bina kisi extra conversion factor ke true banate hain — aur derivation tiny angles ke liye arc ≈ chord par lean karti hai.
Definition Small-angle rule
sin x ≈ x (radians mein)
Ek tiny angle x radians mein measure kiya gaya ho toh angle ka sine almost angle ke equal hota hai:
sin x ≈ x ( for small x ) .
Picture (figure ki right side): arc ke across ek seedha chord dalo. Half-chord r sin ( Δ θ /2 ) hai, jabki half-arc r ( Δ θ /2 ) hai. Ek chhote turn ke liye yeh dono almost coincide karte hain kyunki sin ( Δ θ /2 ) ≈ Δ θ /2 . Toh full chord hai
chord = 2 r sin ( 2 Δ θ ) ≈ 2 r ⋅ 2 Δ θ = r Δ θ .
Swap kitna accurate hai? Error x 3 order ka hai: jaise Δ θ = 0.1 rad (≈ 5. 7 ∘ ) par, sin ( 0.05 ) = 0.0499979 versus 0.05 — 0.01% se bhi kam mismatch. Jaise Δ θ → 0 ratio chord / ( r Δ θ ) → 1 exactly ho jaata hai, yehi wajah hai ki hum ek chhote turn ki limit lete hain.
Figure dekho: magenta arc ki length r Δ θ hai; uske across seedha orange chord almost same length ka hai jab Δ θ tiny hota hai. Yeh "chord ≈ arc" swap — upar sin x ≈ x se justify kiya gaya — woh single trick hai jo velocity triangle ko ∣Δ v ∣ ≈ v Δ θ mein turn karti hai (agla section).
Δ v par apply karna — kyun ∣Δ v ∣ ≈ v Δ θ
Velocity-subtraction figure (§4) par wapas dekho. Do arrows v 1 , v 2 ki same length v hai, toh Δ v ke saath milke woh ek isosceles triangle banate hain — length v ki do equal sides aur unke beech dabba hua chhota angle Δ θ . Us angle ke opposite side Δ v hai, aur woh exactly radius v ki ek chhoti circular fan ka "chord" hai. Bilkul wohi reasoning se,
∣Δ v ∣ = 2 v sin ( 2 Δ θ ) ≈ v Δ θ .
Matlab: velocity mein change hai (uski length v ) times (angle turned Δ θ ) — woh key line jis par parent ki a = v 2 / r derivation tiki hui hai.
ω — angular velocity
ω (Greek omega , seedhe alfazon mein: "kitne radians turn per second") Δ t Δ θ hai. Picture: spoke kitni tez sweep karta hai around, jaise clock ki second-hand. Tez whirl = bada ω .
See Uniform Circular Motion for more on the v = ω r link.
m — mass, aur F — force
m (seedhe alfazon mein: "kitna stuff hai / push karna kitna mushkil hai") ek single number hai. F (seedhe alfazon mein: "ek push ya pull") ek vector hai — ek arrow jiska length strength hai aur jis taraf woh point karta hai woh direction hai jisme woh shove karta hai.
F c — centripetal force (ek naam, koi naya arrow nahi)
F c "required net inward force" ka shorthand hai — saari real forces ke inward slices ka total, kuch nahi. Yeh mass times centripetal acceleration ke equal hai:
F c = m a c = m r v 2 = m ω 2 r .
Dhyan se padho: F c ek requirement hai jo poori karni hai , koi extra force nahi jo tum draw karo. Kisi bhi problem mein tum neeche real providers dhundhte ho aur unka combined inward pull F c ke equal set karte ho. See Newton's Second Law .
Tum inhe situation-by-situation tour mein miloge. Har ek ek real force hai jo shayad inward point kar rahi ho — yaani jo F c ka role play kar rahi ho:
Definition Providers ki quick glossary
T — tension , ek string ka inward pull (Friction ise rubbing se contrast karta hai). Picture: ek taut rope stone ko tumhare haath ki taraf kheench rahi hai.
g — gravitational field strength; m g — weight , Earth ka downward pull.
G , M — Newton's gravitation constant aur ek bada central mass; r 2 GM m ek orbit mein gravity ka inward pull hai. See Gravitation and Orbits .
N — normal force , ek surface jo apne aap ke perpendicular push deti hai. Ek tilted road par uska sideways slice turning karta hai. See Banking of Roads .
f s , μ s — static friction aur uska coefficient; friction at most μ s N supply kar sakta hai tyre slip karne se pehle. See Friction .
q , B — charge aur magnetic field; q v B woh magnetic force hai jo ek charge ko circle mein bend karti hai. See Magnetic Force on Moving Charges .
"centrifugal" — spinning frame mein feel hone wali fake outward force; ground frame mein real nahi. See Pseudo-forces and Non-inertial Frames .
Velocity v tangent to circle
Delta v change of velocity
Small angle rule sin x approx x
Delta v approx v times delta theta
Acceleration a points inward
Centripetal a equals v squared over r
Newton second law F equals m a
Required inward force Fc equals m v squared over r
What real force provides it
Ek vector kaunsi do cheezein store karta hai? Uski size (length) aur uski direction.
∣ v ∣ ka kya matlab hai, aur iska roz ka word kya hai?Velocity arrow ki length — plain speed v .
Circle par velocity arrow kis taraf point karta hai? Circle ke tangent, radius r ke 9 0 ∘ par.
Kisi quantity ke aage Δ ka kya matlab hai? Usmein change: final minus initial.
Δ v constant speed par bhi non-zero kyun hai?Kyunki
v ki direction change hoti hai, toh do arrows equal length ke bawajood differ karte hain.
Small-angle rule batao aur kyun yeh chord ≈ arc allow karta hai. sin x ≈ x small x ke liye radians mein, toh chord = 2 r sin ( Δ θ /2 ) ≈ r Δ θ .
∣Δ v ∣ ≈ v Δ θ kyun hai?Equal-length velocity arrows ek isosceles triangle banate hain;
∣Δ v ∣ = 2 v sin ( Δ θ /2 ) ≈ v Δ θ .
Circular motion mein a kis taraf point karta hai? Center ki taraf (centripetal).
Angle radians mein kyun measure karte hain? Taaki arc length = r θ bina kisi conversion factor ke ho.
ω seedhe alfazon mein kya hai, aur yeh v se kaise link hai?Radians turned per second; v = ω r .
Newton's Second Law ko arrow equation ke roop mein batao. F c kiske liye stand karta hai, aur kya yeh draw karne ke liye ek naya force hai?Net inward force required , F c = m v 2 / r ; koi naya arrow nahi — real forces dwara kiya gaya kaam.