
(a)
Interpretation:
Using the van der Waals constants given in Table 1.6, the molar volumes of krypton, Kr is to be calculated at 25 °C and 1 bar pressure.
Concept introduction:
The

Answer to Problem 1.79E
The molar volumes of (a) krypton, Kr is calculated at 25 °C and 1 bar pressure as follows;
Van der Waals constant for Krypton a = 2.318 atm L2/mol2;
b = 0.03978 L/mol
Boyle temperature,
Molar volume for krypton
Explanation of Solution
The non-ideal gas equation represented as;
In the above equation,
[p+ an2/V2] Correction term introduced for molecular attraction
[V– nb] correction term introduced for volume of molecules
‘a’ and ‘b’ are called as van der Waals constants
a = the pressure correction and it is related to the magnitude and strength of the interactions between gas particles.
b = the volume correction and it is having relationship to the size of the gas particles.
Given;
Van der Waals constant for Krypton a =
Boyle temperature
=
= 711.04 K
At Boyle temperature, the second virial coefficient B is zero. Thus, for one mole of krypton the molar volume is, at one bar pressure
Using the van der Waals constants given in Table 1.6, the molar volumes of krypton, Kr is calculated at 25 °C and 1 bar pressure.
(b)
Interpretation:
Using the van der Waals constants given in Table 1.6, the molar volumes of (b) ethane, C2H6 is to be calculated at 25 °C and 1 bar pressure.
Concept introduction:
The ideal

Answer to Problem 1.79E
The molar volumes of ethane, C2H6 is calculated at 25 °C and 1 bar pressure as follows;
Van der Waals constant for ethane a = 5.489 atm L2/mol2;
b = 0.0638 L/mol
Boyle temperature Tb = a/bR = 1049.5 K
Molar volume for ethane ῡ = RT/p = 87.2 L
Explanation of Solution
The non-ideal gas equation represented as;
In the above equation,
[p + an2/V2] Correction term introduced for molecular attraction
[V – nb] Correction term introduced for volume of molecules
‘a’ and ‘b’ are called as van der Waals constants
a = the pressure correction and it is related to the magnitude and strength of the interactions between gas particles.
b = the volume correction and it is having relationship to the size of the gas particles.
Given;
Van der Waals constant for ethane a = 5.489 atm L2/mol2
b = 0.0638 L/mol
Boyle temperature Tb = a/bR
At Boyle temperature, the second virial coefficient B is zero. Thus, for one mole of ethane the molar volume is, at one bar pressure
ῡ = RT/p
Using the van der Waals constants given in Table 1.6, the molar volumes of ethane, C2H6 is calculated at 25 °C and 1 bar pressure.
(c)
Interpretation:
Using the van der Waals constants given in Table 1.6, the molar volumes of mercury Hg is to be calculated at 25 °C and 1 bar pressure.
Concept introduction:
The ideal gas law considered the molecules of a gas as point particles with perfectly elastic collisions among them in nature. This works importantly well for gases at dilution and at low pressure in many experimental calculations. But the gas molecules are not performing as point masses, and there are situations where the properties of the gas molecules have measurable effect by experiments. Thus, a modification of the ideal gas equation was coined by Johannes D. van der Waals in 1873 to consider size of molecules and the interaction forces among them. It is generally denoted as the van der Waals equation of state.

Answer to Problem 1.79E
The molar volumes of mercury is calculated at 25 °C and 1 bar pressure as follows;
Van der Waals constant for mercury a = 8.093atm L2/mol2;
b = 0.01696 L/mol
Boyle temperature Tb = a/bR = 5822 K
Molar volume for mercury ῡ = RT/p = 484 L
Explanation of Solution
The non-ideal gas equation represented as;
In the above equation,
[p + an2/V2] Correction term introduced for molecular attraction
[V – nb] Correction term introduced for volume of molecules
‘a’ and ‘b’ are called as van der Waals constants
a = the pressure correction and it is related to the magnitude and strength of the interactions between gas particles.
b = the volume correction and it is having relationship to the size of the gas particles.
Given;
Van der Waals constant for mercury a = 8.093atm L2/mol2;
b = 0.01696 L/mol
Boyle temperature Tb = a/bR
= (8.093 atm L2 mol-2)/(0.01696 L mol-1 x 0.08205 L. atm K-1 mol-1
= 5822 K
At Boyle temperature, the second virial coefficient B is zero. Thus, for one mole of mercury the molar volume is, at one bar pressure
ῡ = RT/p
Using the van der Waals constants given in Table 1.6, the molar volumes of mercury Hg is calculated at 25 °C and 1 bar pressure.
Want to see more full solutions like this?
Chapter 1 Solutions
Physical Chemistry
- [Review Topics] [References] Write an acceptable IUPAC name for the compound below. (Only systematic names, not common names are accepted by this question.) Keep the information page open for feedback reference. The IUPAC name is Submit Answer Retry Entire Group 9 more group attempts remainingarrow_forwardPlease draw.arrow_forwardA chromatogram with ideal Gaussian bands has tR = 9.0 minutes and w1/2 = 2.0 minutes. Find the number of theoretical plates that are present, and calculate the height of each theoretical plate if the column is 10 centimeters long.arrow_forward
- An open tubular column has an inner diameter of 207 micrometers, and the thickness of the stationary phase on the inner wall is 0.50 micrometers. Unretained solute passes through in 63 seconds and a particular solute emerges at 433 seconds. Find the distribution constant for this solute and find the fraction of time spent in the stationary phase.arrow_forwardConsider a chromatography column in which Vs= Vm/5. Find the retention factor if Kd= 3 and Kd= 30.arrow_forwardTo improve chromatographic separation, you must: Increase the number of theoretical plates on the column. Increase the height of theoretical plates on the column. Increase both the number and height of theoretical plates on the column. Increasing the flow rate of the mobile phase would Increase longitudinal diffusion Increase broadening due to mass transfer Increase broadening due to multiple paths You can improve the separation of components in gas chromatography by: Rasing the temperature of the injection port Rasing the temperature of the column isothermally Rasing the temperature of the column using temperature programming In GC, separation between two different solutes occurs because the solutes have different solubilities in the mobile phase the solutes volatilize at different rates in the injector the solutes spend different amounts of time in the stationary phasearrow_forward
- please draw and example of the following: Show the base pair connection(hydrogen bond) in DNA and RNAarrow_forwardNaming and drawing secondary Write the systematic (IUPAC) name for each of the following organic molecules: CH3 Z structure CH3 CH2 CH2 N-CH3 CH3-CH2-CH2-CH-CH3 NH CH3-CH-CH2-CH2-CH2-CH2-CH2-CH3 Explanation Check ☐ name ☐ 2025 McGraw Hill LLC. All Rights Reserved. Terms of Use | Privacy C Garrow_forwardC This question shows how molecular orbital (MO) theory can be used to understand the chemical properties of elemental oxygen O₂ and its anionic derivative superoxide Oz. a) Draw the MO energy diagram for both O2 and O2. Clearly label your diagram with atomic orbital names and molecular orbital symmetry labels and include electrons. Draw the Lewis structure of O2. How does the MO description of O2 differ from the Lewis structure, and how does this difference relate to the high reactivity and magnetic properties of oxygen? ) Use the MO diagram in (a) to explain the difference in bond length and bond energy between superoxide ion (Oz, 135 pm, 360 kJ/mol) and oxygen (O2, 120.8 pm, 494 kJ/mol).arrow_forward
- Please drawarrow_forward-Page: 8 nsition metal ions have high-spin aqua complexes except one: [Co(HO)₁]". What is the d-configuration, oxidation state of the metal in [Co(H:O))"? Name and draw the geometry of [Co(H2O)]? b) Draw energy diagrams showing the splitting of the five d orbitals of Co for the two possible electron configurations of [Co(H2O)]: Knowing that A = 16 750 cm and Пl. = 21 000 cm, calculate the configuration energy (.e., balance or ligand-field stabilization energy and pairing energy) for both low spin and high spin configurations of [Co(H2O)]. Which configuration seems more stable at this point of the analysis? (Note that 349.76 cm = 1 kJ/mol) Exchange energy (IT) was not taken into account in part (d), but it plays a role. Assuming exchange an occur within t29 and within eg (but not between tz, and ea), how many exchanges are possible in the low in configuration vs in the high spin configuration? What can you say about the importance of exchange energy 07arrow_forwardDraw everything please on a piece of paper explaining each steparrow_forward
- Chemistry for Engineering StudentsChemistryISBN:9781337398909Author:Lawrence S. Brown, Tom HolmePublisher:Cengage LearningChemistry: Principles and PracticeChemistryISBN:9780534420123Author:Daniel L. Reger, Scott R. Goode, David W. Ball, Edward MercerPublisher:Cengage LearningChemistry: An Atoms First ApproachChemistryISBN:9781305079243Author:Steven S. Zumdahl, Susan A. ZumdahlPublisher:Cengage Learning
- Chemistry: The Molecular ScienceChemistryISBN:9781285199047Author:John W. Moore, Conrad L. StanitskiPublisher:Cengage LearningPhysical ChemistryChemistryISBN:9781133958437Author:Ball, David W. (david Warren), BAER, TomasPublisher:Wadsworth Cengage Learning,





