2.8.11 · D3 · Chemistry › Chemical Kinetics › Reaction mechanisms — elementary steps, rate-determining ste
Yeh page ek workout hai. Hum the parent note ki machinery lete hain aur use har us tarah ke mechanism problem pe chalate hain jo ek exam de sakta hai . Shuru karne se pehle, ek vaada: har symbol kamaya gaya hai. Chalo un do ideas ko phir se anchor karte hain jo tumhe actually chahiye.
Intuition "Rate" ka matlab, picture mein
Socho ek corridor mein log hain jo kai doors ki series se guzarne ki koshish kar rahe hain. Poori bheed ke bahar nikalne ki rate sabse chhote door se set hoti hai — yaani sabse slow step se. Woh chhota door hi rate-determining step (RDS) hai. Is page par sab kuch yahi hai: chhota door dhundho, aur us par intezaar kar rahi bheed ko un cheezein ke terms mein describe karo jo hum actually count kar sakte hain.
Do symbols jo hum baar baar use karte hain:
[ X ] aur constant k
[ X ] ka matlab hai "species X kitni floating around hai ", moles per litre mein measure kiya jata hai (mol L − 1 , likhte hain M ). Ek jar socho: andar zyada dots = bada [ X ] .
k ek rate constant hai — ek fixed number jo kisi given step ke liye given temperature par batata hai "yeh collision kitna eager hai succeed hone ke liye?" Bada k = fast door; chhota k = atka hua peanut-butter jar.
Ek elementary step aA + bB → products ke liye, rate hai k [ A ] a [ B ] b . Exponents ek saath collide karne wale har molecule ki sankhya hain — kyunki simultaneous meeting ki probability multiply hoti hai.
Har mechanism problem in cells mein se ek (ya inhi ka blend) hota hai. Neeche ke hamare 9 examples inhe sab cover karte hain — ek standalone Cell Z bhi hai jo formulas ko unki edges par stress-test karta hai.
Cell
Scenario class
Tricky kyun hai
Example
A
Slow step pehle , usme koi intermediate nahi
"Easy" case — rate seedha padh lo
Ex 1
B
Slow step baad mein , ek fast pre-equilibrium se fed
K ke zariye intermediate eliminate karna padega
Ex 2
C
Intermediate ek reactant hai jo already use ho chuka hai (denominator appear hota hai)
Fast equilibrium ek reactant consume kar rahi hai, isliye woh denominator mein aata hai
Ex 3
D
Unimolecular RDS (molecularity 1)
Degenerate "collision" — ek single molecule toot jaati hai
Ex 4
E
Termolecular / 3-body apparent order
Order 3 tak pahunch sakta hai; kya ek true 3-body step realistic hai?
Ex 5
F
Koi obvious slow step nahi to Steady-State Approximation
Rate build-up/drain balance se set hoti hai, ek door se nahi
Ex 6
G
Real-world word problem (atmospheric / catalysis)
Prose ko steps mein, steps ko law mein translate karo
Ex 7
H
Exam twist : given observed order, sahi valid mechanism chuno
Ulta direction; candidates test karo
Ex 8
Z
Degenerate/limiting checks : zero concentration, huge/tiny k ratios
Kya formulas edges par sane rehte hain?
Ex 9
Worked example Example 1 — clean case
Overall: NO 2 + CO → NO + CO 2
Mechanism:
Step 1 (slow ): NO 2 + NO 2 → NO 3 + NO , rate = k 1 [ NO 2 ] 2
Step 2 (fast): NO 3 + CO → NO 2 + CO 2
Forecast: overall rate law guess karo. Stoichiometry se tempting answer: k [ NO 2 ] [ CO ] . Kya yeh sahi hai?
Step 1 — Chhota door dhundho. Step 1 slow label hai, isliye yeh RDS hai.
Yeh step kyun? Poori bheed utni hi tezi se nikal sakti hai jitna chhota door allow kare. Step 2 fast hai, isliye woh kisi ko rokta nahi.
Step 2 — RDS ki apni stoichiometry se RDS rate likho. Do NO 2 molecules collide karte hain, isliye
Rate = k 1 [ NO 2 ] 2 .
Yeh step kyun? Step 1 elementary hai, isliye exponents = colliding molecules ki sankhya = 2.
Step 3 — Law mein intermediates check karo. NO 3 ek intermediate hai, lekin woh k 1 [ NO 2 ] 2 mein nahi aata. Eliminate karne ko kuch nahi.
Yeh step kyun? Ek finished rate law mein sirf wahi species ho sakti hain jo hum measure kar sakte hain — reactants/products.
Result: Rate = k 1 [ NO 2 ] 2 . NO 2 mein second order, CO mein zero order — CO bilkul appear hi nahi karta!
Verify: Steps sum karo: 2 NO 2 + NO 3 + CO → NO 3 + NO + NO 2 + CO 2 . NO 3 aur ek NO 2 cancel karo: NO 2 + CO → NO + CO 2 ✓ overall se match karta hai. k 1 ki units: rate M s − 1 hai, [ NO 2 ] 2 M 2 hai, isliye k 1 ki units M − 1 s − 1 hain ✓ (ek bimolecular constant).
Yahan hum us trick se milte hain jo is page ka baaki hissa carry karti hai: ek intermediate RDS ke andar baitha hai aur hum use trade karna padte hain.
Figure s01 — Example 2 ka ek diagram. Left mein ek box mein reactants NO + Br2 hain; ek magenta arrow (labelled k 1 , fast) aur ek violet arrow (labelled k − 1 , fast) ki barabar length hain jo ise middle box se connect karti hain jisme intermediate NOBr2 hai. Barabar arrow lengths "forward rate = reverse rate" ki picture hain, yaani equilibrium. Ek patla dotted orange arrow (labelled k 2 , SLOW — chhota door) NOBr2 + NO ko product box 2 NOBr ki taraf leak karta hai.
Worked example Example 2 — pre-equilibrium elimination
Overall: 2 NO + Br 2 → 2 NOBr
Mechanism:
Step 1 (fast equilibrium ): NO + Br 2 ⇌ NOBr 2 , forward k 1 ke saath, reverse k − 1 ke saath
Step 2 (slow ): NOBr 2 + NO → 2 NOBr , rate = k 2 [ NOBr 2 ] [ NO ]
Forecast: NO mein order kya hoga — 1 ya 2? Aage padhne se pehle guess karo; hum Result par iska explicitly jawab dete hain.
Step 1 — RDS rate. Step 2 slow hai:
Rate = k 2 [ NOBr 2 ] [ NO ] .
Kyun: sabse slow door hi pace set karta hai.
Step 2 — Intermediate spot karo. NOBr 2 produce hota hai phir consume hota hai — hum iska bottle nahi khareed sakte. Ise jaana padega.
Kyun: rate laws mein sirf measurable reactants ho sakte hain.
Step 3 — Fast equilibrium use karo. "Fast forward aur reverse" ka matlab hai Step 1 khud ko balance karta hai: forward rate = reverse rate — yeh exactly figure s01 mein equal-length arrows hain.
k 1 [ NO ] [ Br 2 ] = k − 1 [ NOBr 2 ] .
Yeh tool kyun aur koi nahi? Kyunki Step 1 dono directions mein fast hai, yeh equilibrium reach kar leta hai bahut pehle jab slow step use drain kare — isliye equilibrium condition (in-rate = out-rate) hold karti hai.
Step 4 — Intermediate ke liye solve karo.
[ NOBr 2 ] = k − 1 k 1 [ NO ] [ Br 2 ] .
Yeh step kyun? Rate jo hum chahte hain (k 2 [ NOBr 2 ] [ NO ] ) abhi bhi un-measurable [ NOBr 2 ] contain karti hai. Hum equilibrium equation rearrange karte hain taaki [ NOBr 2 ] subject ban jaye — woh hume iske liye ek formula deta hai jo poori tarah measurable reactants se bana hai.
Step 5 — Substitute karo.
Rate = k 2 ⋅ k − 1 k 1 [ NO ] [ Br 2 ] ⋅ [ NO ] = k − 1 k 1 k 2 [ NO ] 2 [ Br 2 ] .
Yeh step kyun? Hum Step-4 expression ko RDS rate mein [ NOBr 2 ] ki jagah drop karte hain, intermediate ko evict karte hain. Jo bachta hai usme sirf NO aur Br 2 hain — woh cheezein jo ek lab measure kar sakti hai. k obs = k 1 k 2 / k − 1 let karo:
Rate = k obs [ NO ] 2 [ Br 2 ] .
Result: forecast ka jawab — NO mein second order , pehla nahi, kyunki do NO molecules path ko feed karte hain (ek equilibrium mein jaata hai, ek slow step mein). Total order 2 + 1 = 3 .
Verify: Sum: NO + Br 2 + NOBr 2 + NO → NOBr 2 + 2 NOBr . NOBr 2 cancel karo: 2 NO + Br 2 → 2 NOBr ✓. k obs ki units: rate M s − 1 hai aur [ NO ] 2 [ Br 2 ] M 3 hai, isliye k obs ki units M − 2 s − 1 hain ✓ (k 1 k 2 / k − 1 ke consistent: units M − 1 s − 1 ⋅ M − 1 s − 1 / s − 1 = M − 2 s − 1 ✓). Numeric spot-check: agar k 1 = 2 , k − 1 = 4 , k 2 = 3 to k obs = 2 ⋅ 3/4 = 1.5 ; [ NO ] = 0.1 , [ Br 2 ] = 0.2 ke saath, Rate = 1.5 ⋅ 0.01 ⋅ 0.2 = 0.003 M s − 1 .
Worked example Example 3 — ek reactant denominator mein chhup jaata hai
Ozone decomposition, 2 O 3 → 3 O 2 :
Step 1 (fast equilibrium ): O 3 ⇌ O 2 + O , k 1 , k − 1
Step 2 (slow ): O + O 3 → 2 O 2 , rate = k 2 [ O ] [ O 3 ]
Forecast: Step 1 ka reverse O 2 khata hai . Kya [ O 2 ] rate law ke upar hoga ya neeche?
Step 1 — RDS rate: Rate = k 2 [ O ] [ O 3 ] .
Step 2 — Intermediate atomic O hai. Use eliminate karo.
Step 3 — Equilibrium condition. Forward = reverse:
k 1 [ O 3 ] = k − 1 [ O 2 ] [ O ] .
Kyun: reverse reaction bimolecular hai (O 2 meets O ), isliye iske rate mein [ O 2 ] factor hota hai — yahi is cell ka poora point hai.
Step 4 — Solve karo.
[ O ] = k − 1 [ O 2 ] k 1 [ O 3 ] .
Yeh step kyun? RDS rate abhi bhi intermediate [ O ] chhupata hai. Hum equilibrium equation rearrange karte hain [ O ] isolate karne ke liye; kyunki [ O 2 ] reverse side par tha, ab woh divide out ho gaya — woh denominator mein slide kar gaya. Yahi precisely woh mechanism hai jisse ek product rate ko inhibit karta hai.
Step 5 — Substitute karo.
Rate = k 2 ⋅ k − 1 [ O 2 ] k 1 [ O 3 ] ⋅ [ O 3 ] = k − 1 k 1 k 2 [ O 2 ] [ O 3 ] 2 .
Yeh step kyun? Step-4 expression ko RDS rate mein drop karne se [ O ] evict ho jaata hai, sirf measurable O 3 aur O 2 bachte hain. k obs = k 1 k 2 / k − 1 let karo:
Rate = k obs [ O 3 ] 2 [ O 2 ] − 1 .
Result: O 3 mein order + 2 , O 2 mein order − 1 . Ek negative order — product O 2 reaction ko inhibit karta hai, exactly wahi jo ozone ke liye experiment dikhata hai.
Verify: Sum: O 3 + O + O 3 → O 2 + O + 2 O 2 . O cancel karo: 2 O 3 → 3 O 2 ✓. k obs ki units: rate M s − 1 = k obs ⋅ M 2 / M = k obs ⋅ M , isliye k obs ki units s − 1 hain ✓ (k 1 k 2 / k − 1 se match: s − 1 ⋅ M − 1 s − 1 / M − 1 s − 1 = s − 1 ✓). Numeric: k 1 = 6 , k − 1 = 3 , k 2 = 2 ⇒ k obs = 4 ; [ O 3 ] = 0.1 , [ O 2 ] = 0.5 ke saath: Rate = 4 ⋅ 0.01/0.5 = 0.08 M s − 1 .
Worked example Example 4 — ek single molecule toot jaati hai
Overall: N 2 O 5 → 2 NO 2 + 2 1 O 2 (simplified). Slow step unimolecular hai:
Step 1 (slow ): N 2 O 5 → NO 2 + NO 3 , rate = k 1 [ N 2 O 5 ]
Step 2 (fast): NO 2 + NO 3 → NO 2 + O 2 + NO … (fast follow-ups)
Forecast: "molecularity 1" ka matlab hai kitne molecules milne chahiye? Order kya hai?
Step 1 — RDS rate. Molecularity = 1 : koi partner nahi chahiye, molecule bas khud hi toot jaata hai.
Rate = k 1 [ N 2 O 5 ] .
Yeh degenerate case kyun hai: "collision" zero partners ke saath matlab hai ek molecule itni vibrational energy reach karta hai ki toot sake — dekho Activation Energy and Catalysts . Exponent 1 hai, 0 nahi: [ N 2 O 5 ] double karne se per second toot sakne wale molecules ki sankhya double ho jaati hai.
Result: Rate = k 1 [ N 2 O 5 ] — first order .
Verify: Units — rate M s − 1 = k 1 ⋅ M , isliye k 1 ki units s − 1 hain ✓ (ek unimolecular constant ki pehchaan). Sanity: [ N 2 O 5 ] = 0 par, Rate = 0 ✓ — decompose karne ko kuch nahi. (Cell Z aise edge tests ko Ex 9 mein aur aage le jaata hai.)
Worked example Example 5 — order kitna high ja sakta hai?
Overall: 2 NO + O 2 → 2 NO 2 . Suppose (hypothetically) ek single termolecular step:
Step 1 (slow , 3-body): NO + NO + O 2 → 2 NO 2 , rate = k 1 [ NO ] 2 [ O 2 ]
Forecast: overall order (exponents ka sum) kya hai? Aur kya ek genuine 3-body collision physically likely hai?
Step 1 — Rate padho. Elementary, molecularity 3:
Rate = k 1 [ NO ] 2 [ O 2 ] , order = 2 + 1 = 3.
Step 2 — Physics par sanity. Teen molecules ka ek hi waqt milna rare hai — yaad karo Collision Theory se ki 2-body collisions bhi norm hain aur 3-body wale roughly hazaar guna kam frequent hote hain. Isliye yeh sahi law deta hai, lekin chemists Example 2 ka pre-equilibrium route prefer karte hain (same law, koi improbable triple collision nahi).
Yeh kyun mention karein? Ek exam dono mechanisms accept kar sakta hai agar dono observed order-3 law reproduce karte hain — lekin tumse flag karne ko kehta hai kaun sa zyada realistic hai.
Result: Rate = k 1 [ NO ] 2 [ O 2 ] , order 3.
Verify: Yeh exactly parent note ke Example 2 ka k obs [ NO ] 2 [ O 2 ] form hai — do alag mechanisms, same rate law , confirm karta hai ki ek rate law ek mechanism uniquely prove nahi kar sakta. k 1 ki units: rate M s − 1 = k 1 ⋅ M 3 , isliye k 1 ki units M − 2 s − 1 hain ✓ (ek termolecular constant). Numeric: k 1 = 5 , [ NO ] = 0.2 , [ O 2 ] = 0.3 : Rate = 5 ⋅ 0.04 ⋅ 0.3 = 0.06 M s − 1 .
Jab koi step "slow" flag nahi hoti, funnel mein do similar doors hote hain. Hum Steady-State Approximation use karte hain: ek reactive intermediate itni tezi se banta aur toot ta hai ki uski matra muskil se change hoti hai, isliye uski net rate of change approximately zero hoti hai .
Figure s02 — time ke against intermediate concentration [ O ] (magenta curve) ka graph. Yeh zero se steeply chadhta hai, phir ek violet dashed plateau par flatten ho jaata hai. Rising part par (orange arrow) yeh destroy hone se zyada tezi se ban raha hai; flat top par (navy arrow) banana aur destroy karna balance karta hai, isliye slope d [ O ] / d t essentially zero hai — woh flat top wahi steady-state assumption hai jo hum use karte hain.
Worked example Example 6 — steady-state derivation
Overall: 2 O 3 → 3 O 2 , lekin ab kuch bhi slow label nahi hai:
Step 1: O 3 k 1 O 2 + O
Step − 1 : O 2 + O k − 1 O 3
Step 2: O + O 3 k 2 2 O 2
Forecast: kya hoga answer ke saath jab k 2 [ O 3 ] , k − 1 [ O 2 ] se bahut chhota ho? Kya yeh Example 3 ke answer pe collapse ho jaana chahiye?
Step 1 — Intermediate O ki net rate likho. Yeh Step 1 se banta hai, Steps − 1 aur 2 se toot ta hai:
d t d [ O ] = k 1 [ O 3 ] − k − 1 [ O 2 ] [ O ] − k 2 [ O ] [ O 3 ] .
Yeh tool kyun? Koi single door narrow nahi hai, isliye hum ek step seedha nahi padh sakte. Balki hum figure s02 mein [ O ] curve ke flat top ko track karte hain: woh chadhta hai, phir level hota hai — us plateau par iska slope approximately zero hai.
Step 2 — Zero set karo (steady state).
k 1 [ O 3 ] = [ O ] ( k − 1 [ O 2 ] + k 2 [ O 3 ] ) ⇒ [ O ] = k − 1 [ O 2 ] + k 2 [ O 3 ] k 1 [ O 3 ] .
Yeh step kyun? Plateau ka matlab hai "banana = toot na", yaani poori right-hand side sum karke zero hoti hai. Use zero set karna ek mushkil differential equation ko ek plain algebraic equation mein badal deta hai, jise hum phir rearrange karte hain un-measurable [ O ] isolate karne ke liye.
Step 3 — Product ki rate (Step 2 ke zariye).
Rate = k 2 [ O ] [ O 3 ] = k − 1 [ O 2 ] + k 2 [ O 3 ] k 1 k 2 [ O 3 ] 2 .
Yeh step kyun? Product O 2 Step 2 mein janam leta hai, isliye uski rate k 2 [ O ] [ O 3 ] hai; hum Step-2 expression for [ O ] substitute karte hain intermediate ko evict karne ke liye, sirf measurable species bachti hain.
Step 4 — Limiting check. Agar k − 1 [ O 2 ] , k 2 [ O 3 ] se bahut zyada hai (reverse fast → pre-equilibrium), k 2 [ O 3 ] denominator se drop karo:
Rate → k − 1 k 1 k 2 [ O 2 ] [ O 3 ] 2 ,
exactly Example 3 — steady state zyada general law hai aur pre-equilibrium uska special case hai.
Verify: Units: numerator k 1 k 2 [ O 3 ] 2 over denominator k − 1 [ O 2 ] deta hai (jaise Ex 3 mein) overall M s − 1 ✓. Numeric, general form ke saath k 1 = 6 , k 2 = 2 , k − 1 = 3 , [ O 3 ] = 0.1 , [ O 2 ] = 0.5 :
Rate = 3 ⋅ 0.5 + 2 ⋅ 0.1 6 ⋅ 2 ⋅ 0.01 = 1.7 0.12 ≈ 0.0706 M s − 1 , Example 3 ke 0.08 ke close (woh sirf denominator mein extra k 2 [ O 3 ] se alag hain) — sensible ✓.
Worked example Example 7 — enzyme-style bottleneck words mein
"Ek enzyme E ek substrate S ko pakad ke bahut jaldi aur reversibly ek complex E S banata hai; phir E S slowly product P mein convert hoti hai, E release karte hue. Rate law sketch karo jab substrate scarce ho."
Step 1 (fast eq): E + S ⇌ E S , k 1 , k − 1
Step 2 (slow): E S k 2 E + P , rate = k 2 [ E S ]
Forecast: bahut zyada enzyme aur thoda sa substrate ke saath, kya tum [ S ] mein first order expect karte ho?
Step 1 — RDS rate. Rate = k 2 [ E S ] .
Step 2 — E S intermediate hai. Step 1 ka fast equilibrium:
k 1 [ E ] [ S ] = k − 1 [ E S ] ⇒ [ E S ] = k − 1 k 1 [ E ] [ S ] .
Yeh step kyun? Hum equilibrium rearrange karte hain un-measurable complex [ E S ] ko enzyme aur substrate ke terms mein isolate karne ke liye jo hum actually monitor kar sakte hain.
Step 3 — Substitute karo.
Rate = k − 1 k 1 k 2 [ E ] [ S ] .
Yeh step kyun? Step-2 expression ko RDS rate mein drop karne se [ E S ] evict hota hai. Scarce-substrate limit mein enzyme mostly free hoti hai, isliye [ E ] nearly ek constant [ E ] 0 hai:
Rate ≈ k ′ [ S ] , k ′ = k − 1 k 1 k 2 [ E ] 0 .
Result: low [ S ] par substrate mein first order — Enzyme Kinetics ka linear low-substrate regime (Michaelis–Menten). High [ S ] par enzyme saturate ho jaata hai aur order 0 ki taraf gir jaata hai (sab enzyme busy — door max flow par jammed open hai).
Verify: Low-[ S ] order = 1 , high-[ S ] order = 0 : scenario matrix ke dono edges capture hue. Numeric low limit: k 1 = 10 , k − 1 = 2 , k 2 = 5 , [ E ] 0 = 0.01 , [ S ] = 0.1 : k ′ = ( 10 ⋅ 5/2 ) ⋅ 0.01 = 0.25 , isliye Rate = 0.25 ⋅ 0.1 = 0.025 M s − 1 .
Worked example Example 8 — woh mechanism chuno jo data fit kare
Experiment H 2 + 2 ICl → I 2 + 2 HCl ke liye Rate = k [ H 2 ] [ ICl ] deta hai. Do candidate mechanisms offer kiye gaye hain. Kaun sa consistent hai?
Candidate X: single step H 2 + 2 ICl → products (termolecular). Predicts Rate = k [ H 2 ] [ ICl ] 2 .
Candidate Y:
Step 1 (slow ): H 2 + ICl → HI + HCl , rate = k 1 [ H 2 ] [ ICl ]
Step 2 (fast): HI + ICl → I 2 + HCl
Forecast: kaun sa predicted law observed k [ H 2 ] [ ICl ] se match karta hai?
Step 1 — X ka law predict karo. Elementary termolecular k [ H 2 ] [ ICl ] 2 deta hai. ICl mein order = 2 . Match nahi karta (observed 1 hai).
Reject kyun: ICl par exponent galat hai, aur 3-body collisions waise bhi unlikely hain.
Step 2 — Y ka law predict karo. RDS Step 1 hai, elementary, deta hai k 1 [ H 2 ] [ ICl ] . ICl mein order = 1 . Match karta hai ✓.
Step 3 — Confirm karo ki Y sahi se sum hota hai. H 2 + ICl + HI + ICl → HI + HCl + I 2 + HCl ; HI cancel karo: H 2 + 2 ICl → I 2 + 2 HCl ✓.
Result: Mechanism Y accept hai (observed law aur stoichiometry fit karta hai; koi improbable termolecular step nahi).
Verify: Observed law order sum = 1 + 1 = 2 ; Y predicts 2 ✓, X predicts 3 ✗. Numeric ke saath k 1 = 4 , [ H 2 ] = 0.5 , [ ICl ] = 0.2 : Rate = 4 ⋅ 0.5 ⋅ 0.2 = 0.4 M s − 1 .
Worked example Example 9 — kya formulas edges par sane rehte hain?
Example 2 ka pre-equilibrium law lo, Rate = k obs [ NO ] 2 [ Br 2 ] ke saath k obs = k 1 k 2 / k − 1 , aur ise chaar edges par stress karo.
Forecast: guess karo kaun sa edge rate ko vanish hone ki jagah blow up karta hai.
Step 1 — Zero reactant. [ NO ] = 0 set karo.
Rate = k obs ⋅ 0 2 ⋅ [ Br 2 ] = 0.
Yeh step kyun? Agar law mein aane wala ek reactant absent hai, to koi path nahi chal sakta — rate exactly zero honi chahiye. Hai ✓.
Step 2 — Ek species ka zero jo law mein nahi hai. Example 1 mein, [ CO ] = 0 set karo: Rate = k 1 [ NO 2 ] 2 unchanged rahti hai.
Yeh step kyun? Zero-order species genuinely RDS ko gate nahi karti, isliye unhe remove karna Step 1 slow nahi kar sakta. Yeh woh counter-intuitive edge hai jis par students trip karte hain.
Step 3 — Bahut fast reverse (k − 1 → ∞ ). k obs = k 1 k 2 / k − 1 mein,
k obs → 0 ⇒ Rate → 0.
Yeh step kyun? Ek zordaar reverse intermediate ko slow step ke use karne se pehle hi tod deta hai — equilibrium far left baithti hai, Step 2 ko starve karti hai. Vanishing rate physically sahi hai ✓.
Step 4 — Product-inhibited law near zero product. Example 3 lo, Rate = k obs [ O 3 ] 2 / [ O 2 ] , aur [ O 2 ] → 0 jaane do.
Rate → + ∞.
Yeh step kyun? Yeh forecast ka "blow-up" edge hai: denominator zero ki taraf jaate hue rate sky-high bhej deta hai. Physically yeh model yahan toot jaata hai (tumhare paas sach mein kabhi zero O 2 nahi hoga, kyunki Step 1 ise banata rehta hai) — ek healthy reminder ki limiting laws ki ek validity domain hoti hai.
Verify: Edge 1 0 deta hai ✓; Edge 2 k 1 [ NO 2 ] 2 ko untouched chhodta hai ✓; Edge 3 0 deta hai ✓ (lim k − 1 → ∞ k 1 k 2 / k − 1 = 0 ); Edge 4 diverge karta hai ✓ (lim [ O 2 ] → 0 + k obs [ O 3 ] 2 / [ O 2 ] = + ∞ ). Chaaron intuition se match karte hain.
Recall Pre-equilibrium vs steady state kab use karein?
Pre-equilibrium tab use karo jab ek fast reversible step clearly slow step ke baad aati hai (reverse forward-drain se bahut zyada hai). Steady-state tab use karo jab koi step slow flag nahi hai, ya safe rehne ke liye — steady-state ek general result hai jo pre-equilibrium ko ek limit ke roop mein contain karta hai.
Recall Negative reaction order kaun se cell se aata hai?
Cell C ::: ek product (ya reactant) jo ek fast equilibrium ke reverse mein appear hota hai denominator mein land karta hai, negative order deta hai — woh species reaction ko inhibit karti hai.
"Slowest sets it, intermediates get evicted." RDS dhundho, uska law likho, phir kisi bhi intermediate ko equilibrium (ya steady state) use karke evict karo jab tak sirf measurable species na bach jaayein.