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Kinetic Energy Distribution Concepts for Understanding Reaction Rate Tutorial

Key Concepts

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Kinetic Energy Distribution Concepts

The kinetic energy of individual N2(g) molecules1 at 273 K (0°C) in a closed vessel was measured in an experiment.
The number of N2(g) molecules with the same kinetic energy was recorded. The results are shown in the table below:

Kinetic Energy
(× 10-3 J)
0 6 23 52 93 140 210 280 370 470 580 700 840 980 1100 1300 1500 1700 1900 2100 2300 5200 Total No. molecules
(× 107)
No. molecules
(× 107)
0 15 40 75 125 180 195 205 200 190 175 150 125 105 75 60 40 25 20 15 13 0 2028

These results were then plotted on a graph as shown below:

Number
of
Molecules
( x 107)
Kinetic Energy Distribution

Kinetic Energy (x 10-3 J)

Notice that all the molecules do not have the same kinetic energy at the same temperature (273 K).
The molecules show a distribution of kinetic energies at the same temperature.

Consider the number of molecules with low kinetic energy, for example, kinetic energy less that 100 × 10-3 J.

Number
of
Molecules
( x 107)
Kinetic Energy Distribution

Kinetic Energy (x 10-3 J)
We could use the data in the table to calculate the number of molecules with kinetic energy less than 100 × 10-3 J:
No. molecules = 0+15+40+75+125
= 255 ( × 107) molecules
or
we could add together the heights of each of the bars in the graph as shown in orange on the graph and arrive at the same result, 255 ( × 107) molecules2.

We can see that the orange area in the bar graph represents the number of molecules with kinetic energy less than 100 × 10-3 J and the blue area in the bar graph represents the number of molecules with kinetic energy greater than 100 × 10-3 J.

The kinetic energy distribution of molecules at a particular temperature can be calculated using equations derived by James Clerk Maxwell and Ludwig Boltzmann in the nineteenth century3.
For this reason, the kinetic energy distribution is referred to as the Maxwell-Boltzmann distribution.

The Maxwell-Boltzmann distribution for our N2(g) molecules at 273 K is shown below:

Number
of
Molecules
( x 107)
Kinetic Energy Distribution
(Maxwell-Boltzmann Distribution)


Kinetic Energy (x 10-3 J)

The solid orange line in the graph is the calculated kinetic energy distribution curve.

The shaded orange area under the curve represents the total number of molecules in the sample.

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Activation Energy and Rates of Reaction Using the Maxwell-Boltzmann Distribution Curve

Activation energy refers to the minimum amount of energy reactant molecules need in order for a successful collision to take place, that is, for a collision that results in a chemical reaction.

Consider a reaction involving N2(g) in which the activation energy is low, for example 200 × 10-3 J.

We can show this activation energy on our graph of the Maxwell-Boltzmann distribution for N2(g) molecules at 273 K as shown below:

Number
of
Molecules
( × 107)
Kinetic Energy Distribution at 273 K
(Maxwell-Boltzmann Distribution)


Kinetic Energy (× 10-3 J)

The graph clearly shows that the orange area under the curve representing the number of molecules with kinetic energy less than 200 × 10-3 J is very much smaller than the blue area under the curve representing the number of molecules with kinetic energy greater than 200 × 10-3 J.

Most of the N2(g) molecules have kinetic energy greater than 200 × 10-3 J.
Since the activation energy for this reaction is 200 × 10-3 J, most of the N2(g) molecules have more than the required energy for successful collisions.
We expect this reaction to take place rapidly at this temperature (273 K).

Now consider a different reaction involving N2(g) in which the activation energy is high, for example 1250 × 10-3 J.

We can represent this much higher activation energy on the same Maxwell-Boltzmann (kinetic energy) distribution for our N2(g) molecules at 273 K as shown below:

Number
of
Molecules
( × 107)
Kinetic Energy Distribution at 273 K
(Maxwell-Boltzmann Distribution)


Kinetic Energy (× 10-3 J)

The graph clearly shows that the orange area under the curve representing the number of molecules with kinetic energy less than 1250 × 10-3 J is very much larger than the blue area under the curve representing the number of molecules with kinetic energy greater than 1250 × 10-3 J.

Few of the N2(g) molecules have kinetic energy greater than 1250 × 10-3 J.
Since the activation energy for this reaction is 1250 × 10-3 J, most of the N2(g) molecules have less than the required energy for successful collisions.
We expect this reaction to take place slowly at this temperature.

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Effect of Temperature on the Maxwell-Boltzmann Distribution Curve

If the sample of N2(g) is heated, then the molecules are expected to move faster, that is, the molecules gain kinetic energy.

The original sample of N2(g) molecules at 273 K (0°C) used above is now heated to 1273 K (1000°C).
The number of N2(g) molecules with the same kinetic energy was recorded, and then graphed as shown below:

Number
of
Molecules
( x 107)
Kinetic Energy Distribution
(Maxwell-Boltzmann Distribution)


Kinetic Energy (x 10-3 J)

Increasing the temperature from 273 K to 1273 K causes a general shift of the kinetic energy distribution for the molecules toward higher kinetic energy.

At the higher temperature, the distribution of kinetic energies of the molecules results in a curve that is broader (less peaked) than the distribution curve at the lower temperature.
At the higher temperature, the molecules display a greater spread (or range) of kinetic energy.

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Effect of Temperature on Rate of Reaction Using Maxwell-Boltzmann Distribution Curve

Consider the reaction involving N2(g) discussed above for which the activation energy was 1250 × 10-3 J.

The activation energy for the reaction, the minimum amount of energy the molecules require in order to collide successfully to produce products, does not change with an increase in temperature, but the kinetic energy each molecule possesses does change with temperature as seen above.

The kinetic energy (Maxwell-Boltzmann) distribution curve for N2(g) molecules at 273 K and 1273 K is plotted and the activation energy (1250 × 10-3 J) is shown in the graph below.

Number
of
Molecules
( × 107)
Kinetic Energy Distribution
(Maxwell-Boltzmann Distribution)


Kinetic Energy (× 10-3 J)

Remember that the area under each curve represents the number of molecules within a given range of kinetic energies.

Let us compare the area under each curve on our graph for the range of kinetic energies between the activation energy and 14000 x 10-3 J in order to describe the relative rate of the reaction at each temperature:

Lower Temperature (273 K) Higher Temperature (1273 K)
Number
of
Molecules
( × 107)
Kinetic Energy Distribution at 273 K
(Maxwell-Boltzmann Distribution)


Kinetic Energy (× 10-3 J)

The blue shaded area under the curve represents the number of molecules with kinetic energy greater than the activation energy.
The area is small, so there are few molecules with kinetic energy greater than the activation energy.
The reaction is expected to be slow at the lower temperature of 273 K.

Number
of
Molecules
( × 107)
Kinetic Energy Distribution at 1273 K
(Maxwell-Boltzmann Distribution)


Kinetic Energy (× 10-3 J)

The blue shaded area under the curve represents the number of molecules with kinetic energy greater than the activation energy.
The area is large, so there are many molecules with kinetic energy greater than the activation energy.
The reaction is expected to be fast at the higher temperature of 1273 K.

More of the molecules have a kinetic energy greater than the activation energy for the reaction at the higher temperature, so the reaction proceeds more rapidly at the higher temperature.

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1. N2(g) is used in this discussion because it is a good approximation of an Ideal Gas.

2. This may look familiar to mathematics students. It is very similar to the mid-ordinate rule used in mathematics to find the approximate area under a curve.

3. The actual equations involved are beyond the scope of a high school chemistry course, we will just use the general shape of the curves in our discussion.