INGENIA

CHM-31

Second-order 1/c

Bimolecular.

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Physical chemistrysecond order

Governing equation

1/c=1/c0+kt1/c=1/c_0+kt

t∈[0,500]t \in \left[0, 500\right]

where

c_0
c0 (M)
k
k (1/M/s)
t
t (s)
c
c (M)

The figure, part by part

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CHM-31 · reactor
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①

Governing law — red

1/c=1/c0+kt1/c=1/c_0+kt

t∈[0,500]t \in \left[0, 500\right]

t=0t = 0c=0.1c = 0.1

②

Domain of the variable — blue

tmin⁡=0,tmax⁡=500t_{\min} = 0,\quad t_{\max} = 500

t∈[0,500]t \in \left[0, 500\right]

t=0t = 0t=0t = 0

③

Response curve — green

1/c=1/c0+kt1/c=1/c_0+kt

t∈[0,500]t \in \left[0, 500\right]

t=0t = 0c=0.1c = 0.1

④

Rate of change — amber

dcdt\frac{\mathrm{d}c}{\mathrm{d}t}

t∈[0,500]t \in \left[0, 500\right]

t=3.145t = 3.145c′=−4.85×10−4c^{\prime} = -4.85\times 10^{-4}

Lecture brief

Historical brief

Ideal-gas law, van ’t Hoff, Nernst, Michaelis–Menten and Clausius–Clapeyron are physical chemistry’s working equations of equilibrium and rate. The lab is pressure, potential and kinetics. This sheet (CHM-31 — Second-order 1/c) is the form associated with second order. Working symbols: c0c_0, kk, tt →\rightarrow cc. Bimolecular.

Purpose

Purpose: compute cc from c0c_0, kk, tt in Physical chemistry via 1/c=1/c0+kt1/c=1/c_0+kt Bimolecular. Use it when a real physical chemistry question must be answered in SI before a code check.

Live realistic example

In symbols

Live case. Given c0=0.100 Mc_0 = 0.100\,\mathrm{M}, k=0.050 1/M/sk = 0.050\,\mathrm{1/M/s}, t=20.000 st = 20.000\,\mathrm{s}, the governing relation 1/c=1/c0+kt1/c=1/c_0+kt yields c=0.0909 Mc = 0.0909\,\mathrm{M}. Bimolecular. Move a slider: the numbers are this situation, not a canned story.

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Inputs

Outputs

  • c c0.0909 M
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CHM-31 · reactor
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Narration of this film

Bimolecular.

Bimolecular.

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