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Physical Chemistry : Thermodynamics, Statistical Mechanics & Kinetics

Andrew Cooksy

Chapter 5

Mass Transport: Collisions and Diffusion - all with Video Answers

Educators


Chapter Questions

02:25

Problem 1

A closed gas cylinder of constant volume and initial temperature of 300 K is heated to 600 K . By what factor do the following parameters change? (a) the most probable speed; (b) the average speed; (c) the mean free path; and (d) the average collision energy

Amy Jiang
Amy Jiang
Numerade Educator
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Problem 2

For the following compounds in the gas phase at 298 K and 1 bar, put a $\sigma$ next to the one with the largest collision cross section, put a $v$ next to the one with the lowest average speed, and put a $\lambda$ next to the one with the largest mean free path.
a. He
b. $\mathrm{C}_6 \mathrm{H}_6$
c. $\mathrm{Cl}_2$

Susan Hallstrom
Susan Hallstrom
Numerade Educator
05:38

Problem 3

When discussing the average kinetic energy, we noted that kinetic energy is a relative quantity, dependent on the relative velocities of the system and the observer. Resolve the following paradox. We consider two molecules, each with mass $m$, with a mutual attractive interaction.
a. In the center of mass frame, the molecules move toward each other with equal speed. At a distance $R_1$ between the molecules, each has speed $v_1$, and at a closer distance $R_0$, the speed of each molecule has doubled to $v_0=2 v_1$.
b. Now we follow exactly the same process, but making our measurements from the standpoint of one of the molecules, which we call the reference. The reference molecule appears to be still, with no kinetic energy, and the other molecule moves toward it at speed $2 v_0$ when at a distance $R_0$, and at a distance $2 v_1=4 v_0$ when at a distance $R_0$.
If energy is conserved in frame (a), the center of mass frame, the potential energy must have decreased by an amount equal to the rise in the kinetic energy:

$$
\begin{aligned}
E_1= & U_1+\frac{m v_1^2}{2}+\frac{m v_1^2}{2}=U_1+m v_1^2 \\
= & E_0=U_0+\frac{m v_0^2}{2}+\frac{m v_0^2}{2}=U_0+4 m v_1^2 ; \\
& U_1-U_0=3 m v_1^2 .
\end{aligned}
$$

Applying the same logic to our measurements in frame (b), however, we find

$$
\begin{gathered}
E_1=U_1+\frac{m\left(2 v_1\right)^2}{2}=U_1+2 m v_1^2 \\
=E_0=U_0+\frac{m\left(2 v_0\right)^2}{2}=U_0+4 m v_1^2 ; \\
U_1-U_0=2 m v_1^2 .
\end{gathered}
$$

Does the shape of the potential energy curve also depend on the choice of reference frame?

Eduard Sanchez
Eduard Sanchez
Numerade Educator
01:08

Problem 4

Section 5.3 finds that a fluid of hard spheres, given enough time, will evenly distribute itself within another fluid of hard spheres. This happens even though the combined fluid after diffusion is at exactly the same energy as before. Identify the driving force for diffusion in this case, from the standpoint of the canonical ensemble of states.

Hunza Gilgit
Hunza Gilgit
Numerade Educator

Problem 5

Which of the following conditions best describes the necessary conditions for separation of two compounds A and B in solution by column chromatography? Let the convection speeds $v$ be such that $v_A>v_B$, let $t_A$ be the time required for compound A to traverse the column (the retention time), and $d$ be the length of the column.
a. $v_{\mathrm{A}} \gg v_{\mathrm{B}}$
b. $v_{\mathrm{A}} D_{\mathrm{A}} \gg v_{\mathrm{B}} D_{\mathrm{B}}$
c. $\frac{v_{\mathrm{A}}}{D_{\mathrm{A}}} \gg \frac{v_{\mathrm{B}}}{D_{\mathrm{B}}}$
d. $v_{\mathrm{A}}-v_{\mathrm{B}} \gg \sqrt{\frac{6}{t_{\mathrm{A}}}}\left(\sqrt{D_{\mathrm{A}}}+\sqrt{D_{\mathrm{B}}}\right)$
e. $d\left(1-\frac{v_{\mathrm{B}}}{v_{\mathrm{A}}}\right) \gg \frac{6 t_{\mathrm{A}}}{v_{\mathrm{A}}}\left(D_{\mathrm{A}}+D_{\mathrm{B}}\right)$
f. $t_{\mathrm{A}}\left(1-\frac{v_{\mathrm{B}}}{v_{\mathrm{A}}}\right)>\sqrt{\frac{6 d}{v_{\mathrm{A}}}}\left(\sqrt{D_{\mathrm{A}}}+\sqrt{D_{\mathrm{B}}}\right)$
g. $\int_0^{t_\lambda} v_{\mathrm{A}} D_{\mathrm{A}} \mathcal{P}_r(r, t) d t \gg \int_0^{v_{\mathrm{A}} t_{\mathrm{A}}} v_{\mathrm{B}} D_{\mathrm{B}} \mathcal{P}_r(r, t) d r$
h. $\int_0^{t_A}\left(\frac{v_A}{D_{\mathrm{A}}}\right) \mathcal{P}_r(r, t) d t \gg \int_0^{v_A t_\lambda}\left(\frac{v_{\mathrm{B}}}{D_{\mathrm{B}}}\right) \mathcal{P}_r(r, t) d r$

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02:43

Problem 6

A sample of $\mathrm{H}_2$ gas is at 298 K and 1.00 bar. Deuterium ( ${ }^2 \mathrm{H}$ ) appears in the sample at its natural abundance of $0.02 \%$. Calculate the collision frequency $\gamma$ in $\mathrm{s}^{-1}$ with which any given $\mathrm{D}_2$ molecule in the sample collides with another $\mathrm{D}_2$ molecule.

Adriano Chikande
Adriano Chikande
Numerade Educator
01:22

Problem 7

We heat a sample of $\mathrm{O}_2$ gas to get an average collision energy of $12.0 \mathrm{~kJ} \mathrm{~mol}^{-1}$. Calculate the temperature and the average relative speed of the $\mathrm{O}_2$ molecules under these conditions.

Lottie Adams
Lottie Adams
Numerade Educator
04:03

Problem 8

Write an equation that could be used to estimate the collision cross section of a molecule from its $b$ van der Waals coefficient. THINKING AHEAD $>$ [What does dimensional analysis suggest about the relationship between $\sigma$ and $b$ ?]

Pronoy Sinha
Pronoy Sinha
Numerade Educator
01:33

Problem 9

Calculate the mean free path for H atoms in warm interstellar atomic clouds, where the temperature is roughly 1000 K and the number density is about $10^3 \mathrm{~cm}^{-3}$. Use $25 \AA^2$ for the collision cross section.

Adriano Chikande
Adriano Chikande
Numerade Educator
01:08

Problem 10

In an equimolar gas mixture of ${ }^4 \mathrm{He}\left(\sigma=22 \AA^2\right)$ and ${ }^{40} \mathrm{Ar}\left(\sigma=36 \AA^2\right)$ at 298 K , out of 1000 collisions suffered by a single typical helium atom, how many of those collisions are with other helium atoms?

Hunza Gilgit
Hunza Gilgit
Numerade Educator
01:18

Problem 11

The median speed $v_{\text {med }}$ is the speed such that there are equal numbers of molecules with speed $v>v_{\text {med }}$ and with speed $v<v_{\text {med }}$. To find the median speed of molecules with mass $m$ at temperature $T$, it is necessary to evaluate a numerical integral. Find an equation that could be solved to find $v_{\text {med }}$; don't bother to solve the numerical integral (it is already solved in Table 5.2).

Lottie Adams
Lottie Adams
Numerade Educator
06:24

Problem 12

Express the average time between molecular collisions $\Delta t$ for a gas-phase molecule in terms of the mean free path $\lambda$ and the average relative velocity $\left(v_{A B}\right)$.

Amit Srivastava
Amit Srivastava
Numerade Educator
02:20

Problem 13

The total number of collisions $N_{\text {coll }}$ in 1 L of $\mathrm{N}_2$ at 273 K and 1.1 bar over a period of 1 s is $1.66 \cdot 10^{35}$. Find $N_{\text {coll }}$ under the following conditions: (a) $100 \mathrm{~cm}^3$, $273 \mathrm{~K}, 1.1 \mathrm{bar}$; (b) $1 \mathrm{~L}, 100 \mathrm{~K}, 1.1$ bar; and (c) $1 \mathrm{~L}, 273 \mathrm{~K}$, 2.2 bar.

Lottie Adams
Lottie Adams
Numerade Educator
02:11

Problem 14

For benzene, the collision cross section $\sigma$ is $88 \AA^2$. Estimate the average collision frequency $\gamma$ for benzene gas at 0.1 bar, 300 K .

Lottie Adams
Lottie Adams
Numerade Educator
04:46

Problem 15

For 300 K , at what number density $\rho$ and mean free path $\lambda$ will benzene have an average collision frequency $\gamma$ comparable to typical intermolecular vibrational frequencies, roughly $10^{12} \mathrm{~s}^{-1}$ ? What does this suggest about benzene at this density?

Sri Datta Vikas Buchemmavari
Sri Datta Vikas Buchemmavari
Numerade Educator
07:58

Problem 16

At what temperature will the collision frequency $\gamma$ be $1.00 \cdot 10^9 \mathrm{~s}^{-1}$ per atom in a sample of $\operatorname{Ar}\left(\sigma=36 \AA^2\right)$ at 1 bar?

Eduard Sanchez
Eduard Sanchez
Numerade Educator
02:27

Problem 17

In a sample of 0.10 mole of $\mathrm{N}_2$ gas at 300 K and 1.00 bar, how many molecular collisions total take place each second?

Adriano Chikande
Adriano Chikande
Numerade Educator
02:41

Problem 18

At what pressure (in bar) does the mean free path in $\mathrm{N}_2\left(\sigma=37 \AA^2\right)$ at 298 K drop to $100 \AA$ ?

Mayukh Banik
Mayukh Banik
Numerade Educator
01:10

Problem 19

From the rotational spectrum of a pure sample of molecule X , it is determined that the mean free path is $9.6 \cdot 10^{-7} \mathrm{~m}$, at a pressure of 0.100 bar and temperature of 298.2 K. Find the collision cross section of X in SI units.

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
02:00

Problem 20

What will be the average speed (not relative speed) of ${ }^{19} \mathrm{~F}_2$ molecules in a sample where the average collision energy is $15.0 \mathrm{~kJ} \mathrm{~mol}^{-1}$ ?

Averell Hause
Averell Hause
Carnegie Mellon University

Problem 21

Assume that the value of $\sigma$ for Ar in Table 5.3 is measured at 298 K . Calculate from this value the effective collision diameter $d$ for Ar. Then, using the parameters in Table 5.2, calculate the classical turning points $R_{\text {class }}(T)$ for the Lennard-Jones potential of Ar at energies corresponding to 298 K and at 998 K above the dissociation limit at $U(R)=0$. Finally, assuming that $d$ is proportional to $R_{\text {class }}(T)$, estimate the value of $\sigma$ if it is measured at 998 K . THINKING AHEAD $>[$ How should the turning points compare to a typical chemical bond length?]

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01:41

Problem 22

Two gas-phase samples of $\mathrm{C}_2 \mathrm{H}_2\left(\sigma=72 \AA^2\right.$, $m=26 \mathrm{amu}$ ), have the same volume and number of moles but different temperatures. Given the values at 300.0 K in the following table, write the corresponding values for 600.0 K , in the same units.

Kristen Justice
Kristen Justice
Numerade Educator
02:06

Problem 23

Two gas-phase samples, $\operatorname{Ar}\left(\sigma=36 \AA^2, m=40 \mathrm{amu}\right)$ and $\mathrm{C}_2 \mathrm{H}_2\left(\sigma=72 \AA^2, m=26 \mathrm{amu}\right)$, have the same pressure and temperature. Given the values for Ar in the following table, write the corresponding values for $\mathrm{C}_2 \mathrm{H}_2$ in the same units.

David Collins
David Collins
Numerade Educator

Problem 24

In experiments on combustion intermediates, highly reactive molecules are formed in the gas phase in a 2.0 m long tube with diameter 75 mm , at total pressures around $500 \mathrm{mtorr}\left(6.6 \cdot 10^{-4} \mathrm{bar}\right)$ and temperatures around 400 K . Assuming the reactive molecules start in the center of the tube and have the mass and collision cross section of $\mathrm{CO}_2$ ( $\sigma=45 \AA^2$ ), calculate the time it takes for the rms travel distance of the molecules to equal the distance to the wall of the tube. This allows an estimate of the lifetime of the intermediates in the system.

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03:50

Problem 25

In an ideal gas sample, $P V$ is one measure of the energy content of the sample ( $P V$ equals the energy needed to fill a vessel to a final volume $V$ at a constant pressure $P$ and at constant temperature). Set $P V_0=\left\langle E_{\mathrm{AB}}\right\rangle$, and find an expression for the characteristic volume $V_0$ in terms of only the mean free path and collision cross section.

Anand Jangid
Anand Jangid
Numerade Educator
03:26

Problem 26

Prove that the average collision energy $\left\langle E_{A A}\right\rangle$ for like molecules still satisfies the equipartition principle. This involves integrals that can be separated into an integral over the relative speed of two molecules $v_{12}$ and an integral over the center of mass speed $v$, where

$$
\left(v_1^2 d v_1\right)\left(v_2^2 d v_2\right)=\left(v^2 d v\right)\left(v_{12}^2 d v_{12}\right)
$$

and

$$
v_1^2+v_2^2=2 v^2+\frac{1}{2} v_{12}^2
$$

Stanley Enemuo
Stanley Enemuo
Numerade Educator
02:11

Problem 27

Some reactions require the simultaneous collision of at least three molecules in order to occur. Assume that for a collision to be characterized as three-body, the collision with the third molecule must occur while the other two molecules are within $4 \AA$ of each other ( $4 \AA$ is the effective radius of an $\mathrm{N}_2$ molecule). Calculate an approximate ratio of three-body to two-body collisions in $\mathrm{N}_2$ gas at 300 K and 1 bar, given that the collision cross section is $43 \AA^2$.

Lottie Adams
Lottie Adams
Numerade Educator
05:02

Problem 28

Find the average collision energy in $\mathrm{kJ} \mathrm{mol}^{-1}$ of a 0.100 mol sample of an ideal gas at 0.831 bar and a volume of 4.00 L .

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
02:03

Problem 29

Experiments in surface science are normally carried out in vacuum chambers at extremely low pressures to prevent the surface from becoming quickly contaminated by stray molecules. Estimate how low the pressure (in bar) must be if a square patch of surface 10.0 nm on a side is to suffer on average fewer than one collision per hour when the temperature is 298 K . Assume the chief contaminant is air and that its molecules have an average speed $\langle v\rangle$ of $650 \mathrm{~m} \mathrm{~s}^{-1}$ and collision cross section of $37 \AA^2$. (The surface is stationary, so you should use $\langle v\rangle$ instead of $\left\langle v_{A A}\right\rangle$.)

Varsha Aggarwal
Varsha Aggarwal
Numerade Educator
01:47

Problem 30

A typical tank of oxygen gas $\left(\sigma=36 \AA^2\right)$ is transported from the seller at 298 K and a pressure of about 170 bar. Find the mean free path in $\AA$.

Lottie Adams
Lottie Adams
Numerade Educator
10:04

Problem 31

To initiate a reaction in chlorine gas, we estimate that we need at least $1.0 \cdot 10^7$ collisions of the chlorine per second, with an average collision energy of at least $7.0 \cdot 10^{-21} \mathrm{~J}$. What are the minimum temperature and pressure (in bar) of chlorine that we should use? Assume the collision cross section is $63 \AA^2$.

Preeti Kumari
Preeti Kumari
Numerade Educator
01:14

Problem 32

If we flip a coin an even number of times $N$, there's a chance that we will get an equal number of heads and tails.
a. Find a general expression for this probability in terms of $N$.
b. Find the minimum number of flips so that this probability is less than $1 / 3$.

Charles Carter
Charles Carter
Numerade Educator
02:56

Problem 33

The text discusses the probabilities $\mathcal{P}(k)$ of the outcomes for three flips of a coin where

$$
k=\text { (number of heads) }- \text { (number of tails). }
$$

Graph the probabilities for six coin flips, and label the axes.

Amany Waheeb
Amany Waheeb
Numerade Educator
01:00

Problem 34

Calculate $\mathcal{P}(k=16)$ for $N=20$ using Eq. 5.26 and compare to the exact solution to show that the approximation is within a factor of 2 of the exact value.

Nick Johnson
Nick Johnson
Numerade Educator
03:16

Problem 35

Using the integral solution to the one-dimensional random walk, calculate the probability that after 100 collisions, a molecule would be (a) where it started, (b) 10 mean free paths from where it started, and (c) 100 mean free paths from where it started.

Chai Santi
Chai Santi
Numerade Educator
02:57

Problem 36

In repeated trials, it is found that molecules starting at the origin in a one-dimensional random walk system have a $2.9 \%$ chance of being found back at the origin after $1.0 \cdot 10^{-3}$ seconds. Estimate the collision frequency $\gamma$.

Christopher Provencher
Christopher Provencher
Numerade Educator
02:13

Problem 37

Calculate the probability that a molecule in a three-dimensional medium will be found between 0.99 and 1.01 cm from its starting point after 1.00 s if the number density is $1.00 \cdot 10^{19} \mathrm{~cm}^{-3}$, the average relative velocity is $1.00 \cdot 10^5 \mathrm{~cm} \mathrm{~s}^{-1}$, and the collision cross section is $100 \AA^2$.

Ma Ednelyn Lim
Ma Ednelyn Lim
Numerade Educator

Problem 38

The diffusion constant for $\mathrm{SF}_6$ in air is $0.150 \mathrm{~cm}^2 \mathrm{~s}^{-1}$ at 373 K . What is the rms distance in cm traveled by $\mathrm{SF}_6$ after 1 hour?

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01:20

Problem 39

The root mean square distance traveled by a radioactive tracer molecule in a sample of nitrogen gas is found to be 65 cm after 2.00 hours. We then double the temperature (in K ) and cut the pressure in half. Estimate the new rms distance covered in 2.00 hours.

David Collins
David Collins
Numerade Educator
00:42

Problem 40

Prove that for a mixture of two gases $A$ and $B$ with constant temperature and constant total pressure everywhere in the sample, the constant $D_{\mathrm{A}}$ for diffusion of A through the mixture must be equal to the constant $D_{\mathrm{B}}$ for diffusion of $B$ through the mixture.

Mishal Gul
Mishal Gul
Numerade Educator
13:30

Problem 41

In Table 5.5, $D_{\text {calc }}$ overestimates the liquid $\mathrm{H}_2 \mathrm{O} /$ acetone diffusion constant by a factor of 26 . Based on this, state a quantitative conclusion about the interaction between $\mathrm{H}_2 \mathrm{O}$ and acetone in the liquid phase.

Chareen Guzman
Chareen Guzman
Numerade Educator
05:30

Problem 42

Write, but do not evaluate, the integral (with all appropriate numerical values) necessary to calculate the fraction of a glycine sample that has diffused in water a distance of at least 5 cm at $20 \mathrm{~s}\left(D=1.055 \cdot 10^{-5} \mathrm{~cm}^2 \mathrm{~s}^{-1}\right)$.

Christopher Provencher
Christopher Provencher
Numerade Educator
02:32

Problem 43

Calculate the diffusion constant of $\mathrm{H}_2 \mathrm{O}$ in liquid $\mathrm{H}_2 \mathrm{O}$ at 298 K , based on our idealized random walk model.

Jerrah Biggerstaff
Jerrah Biggerstaff
Numerade Educator

Problem 44

Write the expression necessary to calculate the average inverse time $1 / t$ for diffusion in three dimensions of the molecules in a sample to a distance $r_0$ from their origin. Take into account that you are probably not starting from a correctly normalized function. (By the way, it is necessary to average $1 / t$ because the average diffusion time is infinite. At infinite time, the molecules are evenly distributed, so-considering only the net motion-some molecules never diffuse away from the origin.)

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Problem 45

Find $\left\langle r^2\right\rangle^{1 / 2}$ in terms of $D$ and $t$ for the case of diffusion across a surface.

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01:22

Problem 46

A long tube is filled with $\mathrm{N}_2$ gas at constant pressure. A small sample of a compound B is introduced at one end of the tube. Write the integral in terms of $D$ and $t$ that you would need to evaluate to find the number of molecules of B flowing past point $Z_0$ midway down the tube between times $t_1$ and $t_2$.

Colin O'Haire
Colin O'Haire
Numerade Educator

Problem 47

For flow in one direction, draw a curve for $\rho(Z)$ near the point $Z_0$ such that
a. the concentration is decreasing as $Z$ increases, and
b. the concentration at $Z_0$ will drop with time.

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02:52

Problem 48

A liquid is added to solvent with an initial (normalized) distribution at $t=0$ of $\mathcal{P}_Z(Z)=A e^{-(Z / a)^5}$, where $A=0.53896 \mathrm{~cm}^{-1}$. This is a nearly constant value from $Z=0$ to $Z= \pm a$, where it rapidly drops to zero, as shown in the graph. Find an expression for the flux as a function of $Z$, and sketch that function on a graph.

Amany Waheeb
Amany Waheeb
Numerade Educator
02:11

Problem 49

The collision cross section for $\mathrm{H}_2$ is $27 \AA^2$ and for benzene is $88 \AA^2$. Which is less viscous at $300 \mathrm{~K}, \mathrm{H}_2$ gas or benzene gas?

Lottie Adams
Lottie Adams
Numerade Educator
01:30

Problem 50

In deriving our equation for the viscosity of a gas, we used a number $N_{\text {coll }}=\rho A\left\langle v_X\right\rangle \Delta t / 2$ for the number of collisions with a certain area $A$ of the wall over time $\Delta t$. If that number is initially $1.00 \cdot 10^8$ for a particular gas, what does it become if we do the following?
a. double the pressure but keep the same temperature
b. double the temperature but keep the same pressure
c. change the molecule to double the collision cross section

Mayukh Banik
Mayukh Banik
Numerade Educator
02:11

Problem 51

For a dense gas, Poiseuille's formula states that $\Delta V / \Delta t$ of a tube with diameter $r$, length $l \ggg r$, and pressure drop $\Delta P$ has the form

$$
\frac{\Delta V}{\Delta t} \propto \frac{\left(r^4 \Delta P\right)}{(\eta l)} .
$$

Estimate how $\Delta V / \Delta t$ depends on each of these parameters $(r, \Delta P, \eta, l)$ in the diffuse gas limit where $l \gg \lambda$, the mean free path.

Ajay Singhal
Ajay Singhal
Numerade Educator
02:41

Problem 52

The Stokes equation, $F_{\text {visc }}=-6 \pi \eta r v$, predicts the viscous force opposing the motion of a spherical particle with radius $r$ at speed $v$ through a medium with viscosity $\eta$. See if you can use the definition of the viscosity to set up a differential equation in the velocity that integrates over the surface of the spherical particle to predict the general form of the Stokes equation (ignoring that factor of 6 ).

Khoobchandra Agrawal
Khoobchandra Agrawal
Numerade Educator
13:38

Problem 53

In a common technique in chemical synthesis, helium is used to carry a volatile mixture out of a reactant flask through two "cold traps" connected in series, as drawn in the following figure. The first trap is cooled by dry ice ( 195 K ) and the second by liquid nitrogen ( 77 K ). The first trap removes water and solvent from the gas, and the isolated product condenses and freezes in the second trap. Indicate by 1,2,3,4, and 5 the order of increasing gas flow rate (in $\mathrm{cm} \mathrm{s}^{-1}$ ) through the tubing in the five different regions (a) through (e) of the apparatus shown, if the pressures change as shown. Assume that the measurements are made in regions of equal cross sectional area $A$ and that the pressures are steady.

Jason Boomer
Jason Boomer
Numerade Educator
04:24

Problem 54

Find the steady state sedimentation speed $v_{s s}$ for sucrose $\left(\mathrm{C}_{12} \mathrm{H}_{22} \mathrm{O}_{11}\right)$ in water $\left(D=5.216 \cdot 10^{-6} \mathrm{~cm}^2 \mathrm{~s}^{-1}\right)$ at 298 K if there is no centrifuge and the only external force working on the molecule is gravity ( $g=980.7 \mathrm{~cm} \mathrm{~s}^{-2}$ ). Use any of the conditions assumed when a centrifuge is used.

Ronald Prasad
Ronald Prasad
Numerade Educator
02:06

Problem 55

Sedimentation is a useful way to measure molecular weight only as long as the sedimentation rate is fast compared to the rate of diffusion. Assume that this can be determined simply by comparing the steady state speed for sedimentation to the diffusion rate $d\left\langle R^2\right\rangle^{1 / 2} / d t$. For what range of diffusion time $t$ is sedimentation useful for a molecule at $T=300 \mathrm{~K}$ with buoyancy correction $b=0.25$, molecular mass $m=25000$ amu, and diffusion constant $D=1.1 \mathrm{~cm}^2 \mathrm{~s}^{-1}$, when placed in an ultracentrifuge 3 cm from the center of rotation and spun at 20000 rpm ?

Kratika Bhadauria
Kratika Bhadauria
Numerade Educator
04:40

Problem 56

Two plots are shown of signal versus distance for the chromatographic separation of two substances at different times. Sketch what the true chromatogram will look like as a function of time if the column is 20 cm long.

Ronald Prasad
Ronald Prasad
Numerade Educator
05:08

Problem 57

In a series of experiments, a gullible professor sits at one end of a long tank of water, tasting the water for evidence of chemicals that are being added at the opposite end. Assume that the professor is equally sensitive to the taste of each chemical. An initial study using sugar finds that it takes 2500 seconds for the professor to detect its presence. In the following table, estimate the amount of time that will elapse before the chemical is detected when the initial experiment is altered in the specified manner. Exact answers may not be possible in all cases. Each experiment is the same as the initial experiment except for the change described.

Niamat Khuda
Niamat Khuda
Numerade Educator
07:38

Problem 58

The diffusion constant of a lysozyme in water is $1.11 \cdot 10^{-6} \mathrm{~cm}^2 \mathrm{~s}^{-1}$, and the diffusion constant of propane in water at the same temperature is $1.21 \cdot 10^{-5} \mathrm{~cm}^2 \mathrm{~s}^{-1}$. If we let propane diffuse in water for $3.60 \cdot 10^3 \mathrm{~s}$ and measure the rms diffusion distance, how long would it take the lysozyme to reach the same rms diffusion distance?

Nicholas Sacco
Nicholas Sacco
Numerade Educator

Problem 59

We add a drop of dye to a solvent in a tube such that the initial distribution is Gaussian along the axis of the tube,

$$
\rho(Z)=A e^{-Z^2 / a^2},
$$

where $A$ and $a$ are constants. Find the flux $J(Z)$ and the rate of change in the number density $d \rho / d t$ both as functions of $Z$. Graph the results.

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