A macromolecule chain with N = 100 and l = 150 ppm is in three dimension. The probability that the ends will be found in 10.0 pm at 3.00 nm distance will be ________.
1.92 × 10-3
This problem asks for the probability of finding the ends of a macromolecule chain within a specific distance range. The macromolecule chain is modeled as a Gaussian chain in three dimensions. The probability density function for the end-to-end distance magnitude \(r\) of a Gaussian chain is given by:
\[P(r) = 4\pi r^2 \left(\frac{3}{2\pi N l^2}\right)^{3/2} e^{-\frac{3r^2}{2N l^2}}\]
Where:
We are given the following values:
The probability of finding the ends within the distance range \(r\) to \(r + \Delta r\) is approximately \(P(r) \Delta r\), assuming \(\Delta r\) is small.
First, let's calculate the term \(Nl^2\):
\(Nl^2 = 100 \times (150 \times 10^{-12} \, \text{m})^2 = 100 \times (22500 \times 10^{-24} \, \text{m}^2) = 2.25 \times 10^{-18} \, \text{m}^2\)
Next, calculate the exponent term argument, \(\frac{3r^2}{2N l^2}\):
\(r^2 = (3.00 \times 10^{-9} \, \text{m})^2 = 9.00 \times 10^{-18} \, \text{m}^2\)
\(\frac{3r^2}{2N l^2} = \frac{3 \times 9.00 \times 10^{-18} \, \text{m}^2}{2 \times 2.25 \times 10^{-18} \, \text{m}^2} = \frac{27.0 \times 10^{-18}}{4.5 \times 10^{-18}} = 6\)
So the exponential term is \(e^{-6}\).
Now, calculate the constant prefactor \(\left(\frac{3}{2\pi N l^2}\right)^{3/2}\). Let \(b = \frac{3}{2N l^2}\):
\(b = \frac{3}{2 \times 2.25 \times 10^{-18} \, \text{m}^2} = \frac{3}{4.5 \times 10^{-18}} \, \text{m}^{-2} = \frac{2}{3} \times 10^{18} \, \text{m}^{-2}\)
The prefactor is \(\left(\frac{b}{\pi}\right)^{3/2}\):
\(\left(\frac{b}{\pi}\right)^{3/2} = \left(\frac{\frac{2}{3} \times 10^{18} \, \text{m}^{-2}}{\pi}\right)^{3/2} = \left(\frac{2}{3\pi} \times 10^{18}\right)^{3/2} \, \text{m}^{-3}\)
Using \(\pi \approx 3.14159\), \(\frac{2}{3\pi} \approx \frac{2}{9.42477} \approx 0.212207\). So, \(\left(\frac{b}{\pi}\right)^{3/2} \approx (0.212207 \times 10^{18})^{1.5} \, \text{m}^{-3} = (0.212207)^{1.5} \times (10^{18})^{1.5} \, \text{m}^{-3} \approx 0.097753 \times 10^{27} \, \text{m}^{-3}\).
Now, calculate the probability density \(P(r)\) at \(r = 3.00 \, \text{nm}\):
\(P(r) = 4\pi r^2 \left(\frac{b}{\pi}\right)^{3/2} e^{-br^2}\)
\(P(r) = 4\pi (9.00 \times 10^{-18} \, \text{m}^2) (0.097753 \times 10^{27} \, \text{m}^{-3}) e^{-6}\)
Using \(e^{-6} \approx 0.00247875\):
\(P(r) \approx 4\pi \times 9 \times 10^{-18} \times 0.097753 \times 10^{27} \times 0.00247875 \, \text{m}^{-1}\)
\(P(r) \approx (36\pi \times 0.097753 \times 0.00247875) \times 10^{(-18+27)} \, \text{m}^{-1}\)
\(P(r) \approx (113.097 \times 0.097753 \times 0.00247875) \times 10^9 \, \text{m}^{-1}\)
\(P(r) \approx (11.0569 \times 0.00247875) \times 10^9 \, \text{m}^{-1}\)
\(P(r) \approx 0.027407 \times 10^9 \, \text{m}^{-1} = 2.7407 \times 10^7 \, \text{m}^{-1}\)
Finally, calculate the probability \(\Delta P = P(r) \Delta r\):
\(\Delta P \approx (2.7407 \times 10^7 \, \text{m}^{-1}) \times (10.0 \times 10^{-12} \, \text{m})\)
\(\Delta P \approx 2.7407 \times 10^{(7 + (-12))} = 2.7407 \times 10^{-5}\)
Let's recheck the multiplication by \(\Delta r\):
\(\Delta P \approx (2.7407 \times 10^7) \times (10 \times 10^{-12}) = 2.7407 \times 10^{7+1-12} = 2.7407 \times 10^{-4}\)
The calculated probability using the standard Gaussian chain model is approximately \(2.74 \times 10^{-4}\).
Reviewing the provided options:
The calculated value \(2.74 \times 10^{-4}\) is closest in magnitude to option 1 \(1.92 \times 10^{-4}\). However, the provided correct answer corresponds to Option 2.
If we assume the intended probability is \(1.92 \times 10^{-3}\), then the corresponding probability density at \(r=3.00 \, \text{nm}\) would need to be \(\frac{1.92 \times 10^{-3}}{10 \times 10^{-12} \, \text{m}} = 1.92 \times 10^8 \, \text{m}^{-1}\). This value is higher than what the standard Gaussian chain formula predicts at this distance.
Based on the standard formula and given parameters, the calculated probability is \(2.74 \times 10^{-4}\).
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