Figure s01 — teen reference triangles. Har triangle ko angle θ se, jo origin par hai, padho: θ ke saamne wali side opposite hai (labelled "opp"), θ ko base par touch karti side adjacent hai (labelled "adj"), aur tedhi side hypotenuse hai (labelled "hyp"). x=asinθ ke liye: opp =x, hyp =a, adj =a2−x2. x=atanθ ke liye: opp =x, adj =a, hyp =a2+x2. x=asecθ ke liye: hyp =x, adj =a, opp =x2−a2. Har back-substitution mein bas in sides ko padhna hota hai.
WHAT hum dekhte hain: radical ke andar ka sign structure — ye akela choice dictate karta hai.
(a)16−x2 ye a2−x2 form hai jisme a=4 (kyunki 42=16). → x=4sinθ, θ∈[−2π,2π], dx=4cosθdθ, root →4cosθ (valid hai kyunki is interval par cosθ≥0).
WHY sine:1−sin2θ=cos2θ ek a2 se shuru hone wale difference ko khatam kar deta hai.
(b)x2+5 ye a2+x2 form hai jisme a=5. → x=5tanθ, θ∈(−2π,2π), dx=5sec2θdθ, root →5secθ (valid hai kyunki is interval par secθ>0).
WHY tangent:1+tan2θ=sec2θ ek sum ko khatam kar deta hai.
(c)x2−9 ye x2−a2 form hai jisme a=3. → x=3secθ, θ∈[0,2π) (x≥3 lete hue), dx=3secθtanθdθ, root →3tanθ (valid hai kyunki is interval par tanθ≥0).
WHY secant:sec2θ−1=tan2θ ek x2 se shuru hone wale difference ko khatam kar deta hai.
Recall Solution L1·2
Step 1 — substitute.x=4sinθ, θ∈[−2π,2π], dx=4cosθdθ. Figure s02 mein sine triangle dekho: opp =x, hyp =4.
Step 2 — root simplify karo.16−x2=16−16sin2θ=16cos2θ=4cosθ.
WHY +4cosθ, koi ∣⋅∣ nahi bachta: generally u2=∣u∣ hota hai, to strictly 16cos2θ=4∣cosθ∣. Lekin chosen range θ∈[−2π,2π] force karti hai cosθ≥0, isliye ∣cosθ∣=cosθ aur bars drop ho jaate hain. Ye hi wajah hai ki range restriction exist karti hai.Step 3 — assemble.dx ka 4cosθ aur root ka 4cosθ cancel ho jaate hain:
∫4cosθ4cosθdθ=∫1dθ=θ+C.WHY ∫1dθ=θ: wo function jiska derivative constant 1 ho, woh θ khud hai (dθdθ=1). Derivative ko ulta padhne se integral milta hai.
Step 4 — back-substitute.sinθ=4x se (Figure s02), θ=arcsin4x — "wo angle jiska sine 4x hai."
∫16−x2dx=arcsin4x+C,x∈(−4,4)Edge/domain note: integrand ko 16−x2>0 chahiye, yani x∈(−4,4); x=±4 par root 0 ho jaata hai aur integrand blow up ho jaata hai, isliye answer strictly andar hi valid hai. Aur arcsin4x khud sirf 4x∈[−1,1] ke liye defined hai — same interval, jo ek acha consistency check hai.
Step 1.a=3, θ∈[−2π,2π]: x=3sinθ, dx=3cosθdθ, 9−x2=3cosθ (bars drop kyunki is range par cosθ≥0), x2=9sin2θ. Wahi sine triangle, Figure s02 with a=3.
Step 2 — saare pieces substitute karo. Yaad raho cscθ=sinθ1 (upar define kiya), isliye sin2θ1=csc2θ:
∫9sin2θ⋅3cosθ3cosθdθ=91∫sin2θdθ=91∫csc2θdθ.WHY ye collapse hua:dx ka cosθ, root ke cosθ se cancel ho gaya — sirf sin mein ek standard integral bachti hai.
Step 3.∫csc2θdθ=−cotθ, to =−91cotθ+C.
WHY ∫csc2θdθ=−cotθ:−cotθ differentiate karo. Kyunki cotθ=sinθcosθ, quotient rule deta hai dθdcotθ=−csc2θ, to dθd(−cotθ)=csc2θ. Ulta padhna integral deta hai.
Step 4 — triangle (Figure s02).sinθ=3x: opposite =x, hyp =3, adjacent =9−x2, isliye cotθ=oppadj=x9−x2.
=−9x9−x2+C,0<∣x∣<3
Recall Solution L2·2
WHY tangent:(x2+4)3/2=(x2+4)3 — ek suma2+x2 hai jisme a=2.
Step 1.x=2tanθ, θ∈(−2π,2π), dx=2sec2θdθ. Is interval par secθ>0, isliye x2+4=2secθ⇒(x2+4)3/2=(2secθ)3=8sec3θ. Tangent triangle, Figure s03 dekho.
Step 2.∫8sec3θ2sec2θdθ=41∫secθdθ=41∫cosθdθ=41sinθ+C.WHY secθ1=cosθ: kyunki secθdefined hai cosθ1 ke roop mein, uska reciprocal cosθ hai. WHY ∫cosθdθ=sinθ:dθdsinθ=cosθ, isliye integrate karna (differentiate ka reverse) sinθ deta hai.
Step 3 — triangle (Figure s03).tanθ=2x: opposite =x, adjacent =2, hyp =x2+4, isliye sinθ=hypopp=x2+4x.
=4x2+4x+C(all real x)
Step 1.a=3, θ∈[0,2π) (x≥3 lete hue): x=3secθ, dx=3secθtanθdθ. Is interval par tanθ≥0, isliye x2−9=9tan2θ=3tanθ (∣⋅∣ drop ho jaata hai kyunki yahan tanθ≥0 hai — upar range table dekho). Secant triangle, Figure s04.
Step 2 — assemble.∫3tanθ⋅3secθtanθdθ=9∫secθtan2θdθ.Step 3 — tan2 ko sec2−1 mein badlo (Pythagorean identities ke through, taaki pieces aise integrals ban jaayein jo hum build kar sakein):
9∫secθ(sec2θ−1)dθ=9∫sec3θdθ−9∫secθdθ.Step 4 — donon sub-integrals KAHAN se aate hain (ye "just known" nahi hain).∫secθdθ ke liye: upar aur neeche (secθ+tanθ) se multiply karo: ∫secθ⋅secθ+tanθsecθ+tanθdθ=∫secθ+tanθsec2θ+secθtanθdθ. Numerator exactly denominator ka derivative hai (dθd(secθ+tanθ)=secθtanθ+sec2θ), isliye ye ∫ww′dθ=ln∣w∣ hai, jo deta hai ∫secθdθ=ln∣secθ+tanθ∣.
∫sec3θdθ ke liye: integration by parts with u=secθ,dv=sec2θdθ se milta hai ∫sec3=secθtanθ−∫secθtan2θ=secθtanθ−∫sec3θ+∫secθ. Is loop ko ∫sec3θ ke liye solve karne par: ∫sec3θdθ=21secθtanθ+21ln∣secθ+tanθ∣.
Step 5 — combine.9(21secθtanθ+21ln∣secθ+tanθ∣)−9ln∣secθ+tanθ∣=29secθtanθ−29ln∣secθ+tanθ∣+C.Step 6 — triangle (Figure s04).secθ=3x, tanθ=3x2−9.
=2xx2−9−29ln3x+x2−9+C
(−29ln3 ko C mein fold kar lo; tum −29ln∣x+x2−9∣+C bhi likh sakte ho.)
Recall Solution L3·2
Step 1.a=2, θ∈[−2π,2π]: x=2sinθ, dx=2cosθdθ, 4−x2=2cosθ (bars drop kyunki cosθ≥0).
Limits convert karo (WHY: back-substitute karne se zyada clean hai):x=0⇒sinθ=0⇒θ=0; x=2⇒sinθ=1⇒θ=2π.
Step 2.∫0π/22cosθ4sin2θ⋅2cosθdθ=4∫0π/2sin2θdθ.Step 3 — power-reduction (dekho Power-reduction & double-angle formulas): sin2θ=21−cos2θ.
WHY ye step:sin2θ ka koi elementary antiderivative "by sight" nahi hai, lekin ye identity ise ek constant plus ek plain cosine mein badal deta hai, dono ek line mein integrate ho jaate hain.
4⋅21∫0π/2(1−cos2θ)dθ=2[θ−21sin2θ]0π/2=2(2π−0)=π.WHY ∫cos2θdθ=21sin2θ:dθd(21sin2θ)=21⋅2cos2θ=cos2θ (chain rule), ulta padhne par.
=πEdge note: upper limit x=2=a par integrand blow up karta hai (root →0), phir bhi area finite hai — θ-integral is improper endpoint ko quietly handle kar leta hai kyunki θ=2π ek bilkul ordinary limit hai.
Step 1 — complete the square (WHY: abhi tak koi bare a2±x2 form nahi hai).
x2+6x+13=(x+3)2+4. Ab ye shifted variable ke saath ek sum hai.
Step 2 — shift phir substitute.u=x+3, du=dx lo. Root =u2+4, a=2: u=2tanθ, θ∈(−2π,2π), du=2sec2θdθ. Is interval par secθ>0, isliye u2+4=2secθ. (Wahi tangent triangle, Figure s03, x→u ke saath.)
Step 3.∫2secθ2sec2θdθ=∫secθdθ=ln∣secθ+tanθ∣+C.WHY ∫secθdθ=ln∣secθ+tanθ∣: exactly wo (secθ+tanθ) se multiply karne wala trick jo L3·1 Step 4 mein derive kiya — numerator denominator ka derivative ban jaata hai.
Step 4 — triangle (Figure s03, x→u).tanθ=2u, secθ=2u2+4.
ln2u2+4+u+C=lnu2+4+u+C(the −ln2 folds into C).Step 5 — u undo karo.=lnx+3+x2+6x+13+C(all real x,since (x+3)2+4>0)
Step 1.a=2, aur kyunki x, 2→2 run karta hai (sab ≥2=a) hum θ∈[0,2π) mein hain: x=2secθ, dx=2secθtanθdθ, x2−2=2tanθ.
WHY +2tanθ:[0,2π) par tanθ≥0 hai, isliye ∣⋅∣ drop ho jaata hai aur root non-negative rehta hai (range table, secant case). Secant triangle, Figure s04 with a=2.
Limits convert karo.x=2⇒secθ=1⇒θ=0; x=2⇒secθ=22=2⇒cosθ=21⇒θ=4π.
Step 2.∫0π/42secθ2tanθ⋅2secθtanθdθ=2∫0π/4tan2θdθ.
Constant track karo: 2secθ2tanθ⋅2secθtanθ=2tan2θ. ✓
Step 3.tan2θ=sec2θ−1⇒∫tan2θdθ=tanθ−θ.
WHY ∫sec2θdθ=tanθ:dθdtanθ=sec2θ, ulta padhne par; aur ∫1dθ=θ.
2[tanθ−θ]0π/4=2(1−4π).=2(1−4π)≈0.303
Recall Solution L5·2
Step 1 — set up.y′=x, isliye L=∫011+x2dx. Ek sum⇒ tangent, a=1.
Step 2.x=tanθ, θ∈(−2π,2π), dx=sec2θdθ. Is interval par secθ>0, isliye 1+x2=secθ.
Limits: x=0→θ=0; x=1→tanθ=1→θ=4π.
L=∫0π/4secθ⋅sec2θdθ=∫0π/4sec3θdθ.Step 3 — ∫sec3 result use karo (L3·1 Step 4 mein parts se derive kiya): ∫sec3θdθ=21secθtanθ+21ln∣secθ+tanθ∣.
θ=4π par: secθ=2, tanθ=1. θ=0 par: donon terms 0.
L=21(2⋅1)+21ln∣2+1∣=22+21ln(2+1).L=22+21ln(1+2)≈1.148
Recall Solution L5·3
Way A — plain u-sub (faster).u=x2+4, du=2xdx lo (dekho Integration by substitution (u-sub)).
∫uxdx=21∫u−1/2du=u=x2+4+C.WHY 21∫u−1/2du=u: power rule ∫undu=n+1un+1 ke saath n=−21 lagate hain to milta hai 1/2u1/2=2u, aage wale 21 se multiply karo =u.
Way B — trig sub (kaam karta hai, lekin heavier).x=2tanθ, θ∈(−2π,2π) isliye secθ>0: ∫2secθ2tanθ2sec2θdθ=2∫tanθsecθdθ=2secθ=2⋅2x2+4=x2+4+C.WHY ∫secθtanθdθ=secθ:dθdsecθ=secθtanθ, ulta padhne par.
**WHY