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1
3105-3108
3 3: Variation in the concentration vs time plot for a zero order reaction Time k = -slope Concentration of R [R ] 0 0 Comparing (3 6) with equation of a straight line, y = mx + c, if we plot [R] against t, we get a straight line (Fig 3
1
3106-3109
3: Variation in the concentration vs time plot for a zero order reaction Time k = -slope Concentration of R [R ] 0 0 Comparing (3 6) with equation of a straight line, y = mx + c, if we plot [R] against t, we get a straight line (Fig 3 3) with slope = –k and intercept equal to [R]0
1
3107-3110
6) with equation of a straight line, y = mx + c, if we plot [R] against t, we get a straight line (Fig 3 3) with slope = –k and intercept equal to [R]0 Further simplifying equation (3
1
3108-3111
3 3) with slope = –k and intercept equal to [R]0 Further simplifying equation (3 6), we get the rate constant, k as [ ] [ ] R0 R k t − = (3
1
3109-3112
3) with slope = –k and intercept equal to [R]0 Further simplifying equation (3 6), we get the rate constant, k as [ ] [ ] R0 R k t − = (3 7) Zero order reactions are relatively uncommon but they occur under special conditions
1
3110-3113
Further simplifying equation (3 6), we get the rate constant, k as [ ] [ ] R0 R k t − = (3 7) Zero order reactions are relatively uncommon but they occur under special conditions Some enzyme catalysed reactions and reactions which occur on metal surfaces are a few examples of zero order reactions
1
3111-3114
6), we get the rate constant, k as [ ] [ ] R0 R k t − = (3 7) Zero order reactions are relatively uncommon but they occur under special conditions Some enzyme catalysed reactions and reactions which occur on metal surfaces are a few examples of zero order reactions The decomposition of gaseous ammonia on a hot platinum surface is a zero order reaction at high pressure
1
3112-3115
7) Zero order reactions are relatively uncommon but they occur under special conditions Some enzyme catalysed reactions and reactions which occur on metal surfaces are a few examples of zero order reactions The decomposition of gaseous ammonia on a hot platinum surface is a zero order reaction at high pressure ( ) ( ) ( ) 1130K 3 2 2 Pt catalyst 2NH g N g +3H g → Rate = k [NH3]0 = k In this reaction, platinum metal acts as a catalyst
1
3113-3116
Some enzyme catalysed reactions and reactions which occur on metal surfaces are a few examples of zero order reactions The decomposition of gaseous ammonia on a hot platinum surface is a zero order reaction at high pressure ( ) ( ) ( ) 1130K 3 2 2 Pt catalyst 2NH g N g +3H g → Rate = k [NH3]0 = k In this reaction, platinum metal acts as a catalyst At high pressure, the metal surface gets saturated with gas molecules
1
3114-3117
The decomposition of gaseous ammonia on a hot platinum surface is a zero order reaction at high pressure ( ) ( ) ( ) 1130K 3 2 2 Pt catalyst 2NH g N g +3H g → Rate = k [NH3]0 = k In this reaction, platinum metal acts as a catalyst At high pressure, the metal surface gets saturated with gas molecules So, a further change in reaction conditions is unable to alter the amount of ammonia on the surface of the catalyst making rate of the reaction independent of its concentration
1
3115-3118
( ) ( ) ( ) 1130K 3 2 2 Pt catalyst 2NH g N g +3H g → Rate = k [NH3]0 = k In this reaction, platinum metal acts as a catalyst At high pressure, the metal surface gets saturated with gas molecules So, a further change in reaction conditions is unable to alter the amount of ammonia on the surface of the catalyst making rate of the reaction independent of its concentration The thermal decomposition of HI on gold surface is another example of zero order reaction
1
3116-3119
At high pressure, the metal surface gets saturated with gas molecules So, a further change in reaction conditions is unable to alter the amount of ammonia on the surface of the catalyst making rate of the reaction independent of its concentration The thermal decomposition of HI on gold surface is another example of zero order reaction In this class of reactions, the rate of the reaction is proportional to the first power of the concentration of the reactant R
1
3117-3120
So, a further change in reaction conditions is unable to alter the amount of ammonia on the surface of the catalyst making rate of the reaction independent of its concentration The thermal decomposition of HI on gold surface is another example of zero order reaction In this class of reactions, the rate of the reaction is proportional to the first power of the concentration of the reactant R For example, R ® P [ ] [ ] d R Rate R d k t = − = or [ ] [ ] d R – d R k t = Integrating this equation, we get ln [R] = – kt + I (3
1
3118-3121
The thermal decomposition of HI on gold surface is another example of zero order reaction In this class of reactions, the rate of the reaction is proportional to the first power of the concentration of the reactant R For example, R ® P [ ] [ ] d R Rate R d k t = − = or [ ] [ ] d R – d R k t = Integrating this equation, we get ln [R] = – kt + I (3 8) Again, I is the constant of integration and its value can be determined easily
1
3119-3122
In this class of reactions, the rate of the reaction is proportional to the first power of the concentration of the reactant R For example, R ® P [ ] [ ] d R Rate R d k t = − = or [ ] [ ] d R – d R k t = Integrating this equation, we get ln [R] = – kt + I (3 8) Again, I is the constant of integration and its value can be determined easily When t = 0, R = [R]0, where [R]0 is the initial concentration of the reactant
1
3120-3123
For example, R ® P [ ] [ ] d R Rate R d k t = − = or [ ] [ ] d R – d R k t = Integrating this equation, we get ln [R] = – kt + I (3 8) Again, I is the constant of integration and its value can be determined easily When t = 0, R = [R]0, where [R]0 is the initial concentration of the reactant Therefore, equation (3
1
3121-3124
8) Again, I is the constant of integration and its value can be determined easily When t = 0, R = [R]0, where [R]0 is the initial concentration of the reactant Therefore, equation (3 8) can be written as ln [R]0 = –k × 0 + I ln [R]0 = I Substituting the value of I in equation (3
1
3122-3125
When t = 0, R = [R]0, where [R]0 is the initial concentration of the reactant Therefore, equation (3 8) can be written as ln [R]0 = –k × 0 + I ln [R]0 = I Substituting the value of I in equation (3 8) ln[R] = –kt + ln[R]0 (3
1
3123-3126
Therefore, equation (3 8) can be written as ln [R]0 = –k × 0 + I ln [R]0 = I Substituting the value of I in equation (3 8) ln[R] = –kt + ln[R]0 (3 9) 3
1
3124-3127
8) can be written as ln [R]0 = –k × 0 + I ln [R]0 = I Substituting the value of I in equation (3 8) ln[R] = –kt + ln[R]0 (3 9) 3 3
1
3125-3128
8) ln[R] = –kt + ln[R]0 (3 9) 3 3 2 First Order Reactions Rationalised 2023-24 73 Chemical Kinetics Rearranging this equation [ ] [ ]0 lnR R kt = − or     1 lnR0 R k t (3
1
3126-3129
9) 3 3 2 First Order Reactions Rationalised 2023-24 73 Chemical Kinetics Rearranging this equation [ ] [ ]0 lnR R kt = − or     1 lnR0 R k t (3 10) At time t1 from equation (3
1
3127-3130
3 2 First Order Reactions Rationalised 2023-24 73 Chemical Kinetics Rearranging this equation [ ] [ ]0 lnR R kt = − or     1 lnR0 R k t (3 10) At time t1 from equation (3 8) *ln[R]1 = – kt1 + *ln[R]0 (3
1
3128-3131
2 First Order Reactions Rationalised 2023-24 73 Chemical Kinetics Rearranging this equation [ ] [ ]0 lnR R kt = − or     1 lnR0 R k t (3 10) At time t1 from equation (3 8) *ln[R]1 = – kt1 + *ln[R]0 (3 11) At time t2 ln[R]2 = – kt2 + ln[R]0 (3
1
3129-3132
10) At time t1 from equation (3 8) *ln[R]1 = – kt1 + *ln[R]0 (3 11) At time t2 ln[R]2 = – kt2 + ln[R]0 (3 12) where, [R]1 and [R]2 are the concentrations of the reactants at time t1 and t2 respectively
1
3130-3133
8) *ln[R]1 = – kt1 + *ln[R]0 (3 11) At time t2 ln[R]2 = – kt2 + ln[R]0 (3 12) where, [R]1 and [R]2 are the concentrations of the reactants at time t1 and t2 respectively Subtracting (3
1
3131-3134
11) At time t2 ln[R]2 = – kt2 + ln[R]0 (3 12) where, [R]1 and [R]2 are the concentrations of the reactants at time t1 and t2 respectively Subtracting (3 12) from (3
1
3132-3135
12) where, [R]1 and [R]2 are the concentrations of the reactants at time t1 and t2 respectively Subtracting (3 12) from (3 11) ln[R]1– ln[R]2 = – kt1 – (–kt2) [ ] [ ] ( ) − = 1 2 1 2 lnR R t t k ( ) [ ] [ ] 1 2 1 2 1 R ln R k t t = − (3
1
3133-3136
Subtracting (3 12) from (3 11) ln[R]1– ln[R]2 = – kt1 – (–kt2) [ ] [ ] ( ) − = 1 2 1 2 lnR R t t k ( ) [ ] [ ] 1 2 1 2 1 R ln R k t t = − (3 13) Equation (3
1
3134-3137
12) from (3 11) ln[R]1– ln[R]2 = – kt1 – (–kt2) [ ] [ ] ( ) − = 1 2 1 2 lnR R t t k ( ) [ ] [ ] 1 2 1 2 1 R ln R k t t = − (3 13) Equation (3 9) can also be written as [[ ] ] = − 0 R ln R kt Taking antilog of both sides [R] = [R]0 e–kt (3
1
3135-3138
11) ln[R]1– ln[R]2 = – kt1 – (–kt2) [ ] [ ] ( ) − = 1 2 1 2 lnR R t t k ( ) [ ] [ ] 1 2 1 2 1 R ln R k t t = − (3 13) Equation (3 9) can also be written as [[ ] ] = − 0 R ln R kt Taking antilog of both sides [R] = [R]0 e–kt (3 14) Comparing equation (3
1
3136-3139
13) Equation (3 9) can also be written as [[ ] ] = − 0 R ln R kt Taking antilog of both sides [R] = [R]0 e–kt (3 14) Comparing equation (3 9) with y = mx + c, if we plot ln [R] against t (Fig
1
3137-3140
9) can also be written as [[ ] ] = − 0 R ln R kt Taking antilog of both sides [R] = [R]0 e–kt (3 14) Comparing equation (3 9) with y = mx + c, if we plot ln [R] against t (Fig 3
1
3138-3141
14) Comparing equation (3 9) with y = mx + c, if we plot ln [R] against t (Fig 3 4) we get a straight line with slope = –k and intercept equal to ln [R]0 The first order rate equation (3
1
3139-3142
9) with y = mx + c, if we plot ln [R] against t (Fig 3 4) we get a straight line with slope = –k and intercept equal to ln [R]0 The first order rate equation (3 10) can also be written in the form [ ] [ ] 2
1
3140-3143
3 4) we get a straight line with slope = –k and intercept equal to ln [R]0 The first order rate equation (3 10) can also be written in the form [ ] [ ] 2 303 logR0 R k t = (3
1
3141-3144
4) we get a straight line with slope = –k and intercept equal to ln [R]0 The first order rate equation (3 10) can also be written in the form [ ] [ ] 2 303 logR0 R k t = (3 15) * [ ] [ ] logR0 2
1
3142-3145
10) can also be written in the form [ ] [ ] 2 303 logR0 R k t = (3 15) * [ ] [ ] logR0 2 303 R kt = If we plot a graph between log [R]0/[R] vs t, (Fig
1
3143-3146
303 logR0 R k t = (3 15) * [ ] [ ] logR0 2 303 R kt = If we plot a graph between log [R]0/[R] vs t, (Fig 3
1
3144-3147
15) * [ ] [ ] logR0 2 303 R kt = If we plot a graph between log [R]0/[R] vs t, (Fig 3 5), the slope = k/2
1
3145-3148
303 R kt = If we plot a graph between log [R]0/[R] vs t, (Fig 3 5), the slope = k/2 303 Hydrogenation of ethene is an example of first order reaction
1
3146-3149
3 5), the slope = k/2 303 Hydrogenation of ethene is an example of first order reaction C2H4(g) + H2 (g) ® C2H6(g) Rate = k [C2H4] All natural and artificial radioactive decay of unstable nuclei take place by first order kinetics
1
3147-3150
5), the slope = k/2 303 Hydrogenation of ethene is an example of first order reaction C2H4(g) + H2 (g) ® C2H6(g) Rate = k [C2H4] All natural and artificial radioactive decay of unstable nuclei take place by first order kinetics * Refer to Appendix-IV for ln and log (logarithms)
1
3148-3151
303 Hydrogenation of ethene is an example of first order reaction C2H4(g) + H2 (g) ® C2H6(g) Rate = k [C2H4] All natural and artificial radioactive decay of unstable nuclei take place by first order kinetics * Refer to Appendix-IV for ln and log (logarithms) Rationalised 2023-24 74 Chemistry Fig
1
3149-3152
C2H4(g) + H2 (g) ® C2H6(g) Rate = k [C2H4] All natural and artificial radioactive decay of unstable nuclei take place by first order kinetics * Refer to Appendix-IV for ln and log (logarithms) Rationalised 2023-24 74 Chemistry Fig 3
1
3150-3153
* Refer to Appendix-IV for ln and log (logarithms) Rationalised 2023-24 74 Chemistry Fig 3 4: A plot between ln[R] and t for a first order reaction Fig
1
3151-3154
Rationalised 2023-24 74 Chemistry Fig 3 4: A plot between ln[R] and t for a first order reaction Fig 3
1
3152-3155
3 4: A plot between ln[R] and t for a first order reaction Fig 3 5: Plot of log [R]0/[R] vs time for a first order reaction Slope = /2
1
3153-3156
4: A plot between ln[R] and t for a first order reaction Fig 3 5: Plot of log [R]0/[R] vs time for a first order reaction Slope = /2 303 k log ([R /[R]) 0] Time 0 226 4 222 88 2 86 Ra He Rn   Rate = k [Ra] Decomposition of N2O5 and N2O are some more examples of first order reactions
1
3154-3157
3 5: Plot of log [R]0/[R] vs time for a first order reaction Slope = /2 303 k log ([R /[R]) 0] Time 0 226 4 222 88 2 86 Ra He Rn   Rate = k [Ra] Decomposition of N2O5 and N2O are some more examples of first order reactions The initial concentration of N2O5 in the following first order reaction N2O5(g) ® 2 NO2(g) + 1/2O2 (g) was 1
1
3155-3158
5: Plot of log [R]0/[R] vs time for a first order reaction Slope = /2 303 k log ([R /[R]) 0] Time 0 226 4 222 88 2 86 Ra He Rn   Rate = k [Ra] Decomposition of N2O5 and N2O are some more examples of first order reactions The initial concentration of N2O5 in the following first order reaction N2O5(g) ® 2 NO2(g) + 1/2O2 (g) was 1 24 × 10–2 mol L–1 at 318 K
1
3156-3159
303 k log ([R /[R]) 0] Time 0 226 4 222 88 2 86 Ra He Rn   Rate = k [Ra] Decomposition of N2O5 and N2O are some more examples of first order reactions The initial concentration of N2O5 in the following first order reaction N2O5(g) ® 2 NO2(g) + 1/2O2 (g) was 1 24 × 10–2 mol L–1 at 318 K The concentration of N2O5 after 60 minutes was 0
1
3157-3160
The initial concentration of N2O5 in the following first order reaction N2O5(g) ® 2 NO2(g) + 1/2O2 (g) was 1 24 × 10–2 mol L–1 at 318 K The concentration of N2O5 after 60 minutes was 0 20 × 10–2 mol L–1
1
3158-3161
24 × 10–2 mol L–1 at 318 K The concentration of N2O5 after 60 minutes was 0 20 × 10–2 mol L–1 Calculate the rate constant of the reaction at 318 K
1
3159-3162
The concentration of N2O5 after 60 minutes was 0 20 × 10–2 mol L–1 Calculate the rate constant of the reaction at 318 K For a first order reaction     1 2 R log R =   2 1 2
1
3160-3163
20 × 10–2 mol L–1 Calculate the rate constant of the reaction at 318 K For a first order reaction     1 2 R log R =   2 1 2 303 k t t  k =       1 2 1 2 t2
1
3161-3164
Calculate the rate constant of the reaction at 318 K For a first order reaction     1 2 R log R =   2 1 2 303 k t t  k =       1 2 1 2 t2 303 log R t R  =   2 1 2 1 1
1
3162-3165
For a first order reaction     1 2 R log R =   2 1 2 303 k t t  k =       1 2 1 2 t2 303 log R t R  =   2 1 2 1 1 24 10 mol L 2
1
3163-3166
303 k t t  k =       1 2 1 2 t2 303 log R t R  =   2 1 2 1 1 24 10 mol L 2 303 60 min 0 minlog 0
1
3164-3167
303 log R t R  =   2 1 2 1 1 24 10 mol L 2 303 60 min 0 minlog 0 20 10 mol L        = 1 2
1
3165-3168
24 10 mol L 2 303 60 min 0 minlog 0 20 10 mol L        = 1 2 303 log 6
1
3166-3169
303 60 min 0 minlog 0 20 10 mol L        = 1 2 303 log 6 2 min 60  k = 0
1
3167-3170
20 10 mol L        = 1 2 303 log 6 2 min 60  k = 0 0304 min-1 Example 3
1
3168-3171
303 log 6 2 min 60  k = 0 0304 min-1 Example 3 5 Example 3
1
3169-3172
2 min 60  k = 0 0304 min-1 Example 3 5 Example 3 5 Example 3
1
3170-3173
0304 min-1 Example 3 5 Example 3 5 Example 3 5 Example 3
1
3171-3174
5 Example 3 5 Example 3 5 Example 3 5 Example 3
1
3172-3175
5 Example 3 5 Example 3 5 Example 3 5 Solution Solution Solution Solution Solution Let us consider a typical first order gas phase reaction A(g) ® B(g) + C(g) Let pi be the initial pressure of A and pt the total pressure at time ‘t’
1
3173-3176
5 Example 3 5 Example 3 5 Solution Solution Solution Solution Solution Let us consider a typical first order gas phase reaction A(g) ® B(g) + C(g) Let pi be the initial pressure of A and pt the total pressure at time ‘t’ Integrated rate equation for such a reaction can be derived as Total pressure pt = pA + pB + pC (pressure units) Rationalised 2023-24 75 Chemical Kinetics pA, pB and pC are the partial pressures of A, B and C, respectively
1
3174-3177
5 Example 3 5 Solution Solution Solution Solution Solution Let us consider a typical first order gas phase reaction A(g) ® B(g) + C(g) Let pi be the initial pressure of A and pt the total pressure at time ‘t’ Integrated rate equation for such a reaction can be derived as Total pressure pt = pA + pB + pC (pressure units) Rationalised 2023-24 75 Chemical Kinetics pA, pB and pC are the partial pressures of A, B and C, respectively If x atm be the decrease in pressure of A at time t and one mole each of B and C is being formed, the increase in pressure of B and C will also be x atm each
1
3175-3178
5 Solution Solution Solution Solution Solution Let us consider a typical first order gas phase reaction A(g) ® B(g) + C(g) Let pi be the initial pressure of A and pt the total pressure at time ‘t’ Integrated rate equation for such a reaction can be derived as Total pressure pt = pA + pB + pC (pressure units) Rationalised 2023-24 75 Chemical Kinetics pA, pB and pC are the partial pressures of A, B and C, respectively If x atm be the decrease in pressure of A at time t and one mole each of B and C is being formed, the increase in pressure of B and C will also be x atm each A(g) ® B(g) + C(g) At t = 0 pi atm 0 atm 0 atm At time t (pi–x) atm x atm x atm where, pi is the initial pressure at time t = 0
1
3176-3179
Integrated rate equation for such a reaction can be derived as Total pressure pt = pA + pB + pC (pressure units) Rationalised 2023-24 75 Chemical Kinetics pA, pB and pC are the partial pressures of A, B and C, respectively If x atm be the decrease in pressure of A at time t and one mole each of B and C is being formed, the increase in pressure of B and C will also be x atm each A(g) ® B(g) + C(g) At t = 0 pi atm 0 atm 0 atm At time t (pi–x) atm x atm x atm where, pi is the initial pressure at time t = 0 pt = (pi – x) + x + x = pi + x x = (pt - pi) where, pA = pi – x = pi – (pt – pi) = 2pi – pt k = i A 2
1
3177-3180
If x atm be the decrease in pressure of A at time t and one mole each of B and C is being formed, the increase in pressure of B and C will also be x atm each A(g) ® B(g) + C(g) At t = 0 pi atm 0 atm 0 atm At time t (pi–x) atm x atm x atm where, pi is the initial pressure at time t = 0 pt = (pi – x) + x + x = pi + x x = (pt - pi) where, pA = pi – x = pi – (pt – pi) = 2pi – pt k = i A 2 303 log p p t           (3
1
3178-3181
A(g) ® B(g) + C(g) At t = 0 pi atm 0 atm 0 atm At time t (pi–x) atm x atm x atm where, pi is the initial pressure at time t = 0 pt = (pi – x) + x + x = pi + x x = (pt - pi) where, pA = pi – x = pi – (pt – pi) = 2pi – pt k = i A 2 303 log p p t           (3 16) =   i i t 2
1
3179-3182
pt = (pi – x) + x + x = pi + x x = (pt - pi) where, pA = pi – x = pi – (pt – pi) = 2pi – pt k = i A 2 303 log p p t           (3 16) =   i i t 2 303 log 2 p p p t  The following data were obtained during the first order thermal decomposition of N2O5 (g) at constant volume: ( ) ( ) ( ) 2 5 2 4 2 g g g 2N O 2N O O → + S
1
3180-3183
303 log p p t           (3 16) =   i i t 2 303 log 2 p p p t  The following data were obtained during the first order thermal decomposition of N2O5 (g) at constant volume: ( ) ( ) ( ) 2 5 2 4 2 g g g 2N O 2N O O → + S No
1
3181-3184
16) =   i i t 2 303 log 2 p p p t  The following data were obtained during the first order thermal decomposition of N2O5 (g) at constant volume: ( ) ( ) ( ) 2 5 2 4 2 g g g 2N O 2N O O → + S No Time/s Total Pressure/(atm) 1
1
3182-3185
303 log 2 p p p t  The following data were obtained during the first order thermal decomposition of N2O5 (g) at constant volume: ( ) ( ) ( ) 2 5 2 4 2 g g g 2N O 2N O O → + S No Time/s Total Pressure/(atm) 1 0 0
1
3183-3186
No Time/s Total Pressure/(atm) 1 0 0 5 2
1
3184-3187
Time/s Total Pressure/(atm) 1 0 0 5 2 100 0
1
3185-3188
0 0 5 2 100 0 512 Calculate the rate constant
1
3186-3189
5 2 100 0 512 Calculate the rate constant Let the pressure of N2O5(g) decrease by 2x atm
1
3187-3190
100 0 512 Calculate the rate constant Let the pressure of N2O5(g) decrease by 2x atm As two moles of N2O5 decompose to give two moles of N2O4(g) and one mole of O2 (g), the pressure of N2O4 (g) increases by 2x atm and that of O2 (g) increases by x atm
1
3188-3191
512 Calculate the rate constant Let the pressure of N2O5(g) decrease by 2x atm As two moles of N2O5 decompose to give two moles of N2O4(g) and one mole of O2 (g), the pressure of N2O4 (g) increases by 2x atm and that of O2 (g) increases by x atm ( ) ( ) ( ) 2 5 2 4 2 g g g 2N O 2N O O → + Start t = 0 0
1
3189-3192
Let the pressure of N2O5(g) decrease by 2x atm As two moles of N2O5 decompose to give two moles of N2O4(g) and one mole of O2 (g), the pressure of N2O4 (g) increases by 2x atm and that of O2 (g) increases by x atm ( ) ( ) ( ) 2 5 2 4 2 g g g 2N O 2N O O → + Start t = 0 0 5 atm 0 atm 0 atm At time t (0
1
3190-3193
As two moles of N2O5 decompose to give two moles of N2O4(g) and one mole of O2 (g), the pressure of N2O4 (g) increases by 2x atm and that of O2 (g) increases by x atm ( ) ( ) ( ) 2 5 2 4 2 g g g 2N O 2N O O → + Start t = 0 0 5 atm 0 atm 0 atm At time t (0 5 – 2x) atm 2x atm x atm pt = 2 5 2 4 2 N O N O O p p p   = (0
1
3191-3194
( ) ( ) ( ) 2 5 2 4 2 g g g 2N O 2N O O → + Start t = 0 0 5 atm 0 atm 0 atm At time t (0 5 – 2x) atm 2x atm x atm pt = 2 5 2 4 2 N O N O O p p p   = (0 5 – 2x) + 2x + x = 0
1
3192-3195
5 atm 0 atm 0 atm At time t (0 5 – 2x) atm 2x atm x atm pt = 2 5 2 4 2 N O N O O p p p   = (0 5 – 2x) + 2x + x = 0 5 + x x 0
1
3193-3196
5 – 2x) atm 2x atm x atm pt = 2 5 2 4 2 N O N O O p p p   = (0 5 – 2x) + 2x + x = 0 5 + x x 0 5 tp = − 2 pN O5 = 0
1
3194-3197
5 – 2x) + 2x + x = 0 5 + x x 0 5 tp = − 2 pN O5 = 0 5 – 2x = 0
1
3195-3198
5 + x x 0 5 tp = − 2 pN O5 = 0 5 – 2x = 0 5 – 2 (pt – 0
1
3196-3199
5 tp = − 2 pN O5 = 0 5 – 2x = 0 5 – 2 (pt – 0 5) = 1
1
3197-3200
5 – 2x = 0 5 – 2 (pt – 0 5) = 1 5 – 2pt At t = 100 s; pt = 0
1
3198-3201
5 – 2 (pt – 0 5) = 1 5 – 2pt At t = 100 s; pt = 0 512 atm Example 3
1
3199-3202
5) = 1 5 – 2pt At t = 100 s; pt = 0 512 atm Example 3 6 Example 3
1
3200-3203
5 – 2pt At t = 100 s; pt = 0 512 atm Example 3 6 Example 3 6 Example 3
1
3201-3204
512 atm Example 3 6 Example 3 6 Example 3 6 Example 3
1
3202-3205
6 Example 3 6 Example 3 6 Example 3 6 Example 3
1
3203-3206
6 Example 3 6 Example 3 6 Example 3 6 Solution Solution Solution Solution Solution Rationalised 2023-24 76 Chemistry The half-life of a reaction is the time in which the concentration of a reactant is reduced to one half of its initial concentration
1
3204-3207
6 Example 3 6 Example 3 6 Solution Solution Solution Solution Solution Rationalised 2023-24 76 Chemistry The half-life of a reaction is the time in which the concentration of a reactant is reduced to one half of its initial concentration It is represented as t1/2