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Molar heat capacity of a gas does not depend on (a) its temperature (b) its molecular weight (c) its atomicity (d) the conditions under which heat is supplied

Short Answer

Expert verified
Molar heat capacity does not depend on the molecular weight.

Step by step solution

01

Understand the Concept of Molar Heat Capacity

Molar heat capacity is the amount of heat required to raise the temperature of one mole of a substance by one degree Celsius. It is typically denoted in units of J/(mol·K).
02

Analyze Each Option

Consider each option: - (a) Temperature: Molar heat capacity can depend on temperature, especially for gases where heat capacity changes with temperature variably. - (b) Molecular Weight: Molar heat capacity is independent of molecular weight since it is a property per mole. - (c) Atomicity: Molar heat capacity varies with atomicity (number of atoms in a molecule) as it affects the degrees of freedom. - (d) Conditions: It does depend on conditions such as constant volume or constant pressure due to different processes (isothermal, adiabatic, etc.).
03

Identify the Correct Answer

After evaluating, the molar heat capacity does not depend on the molecular weight (b). This is because molar properties are defined per mole, making them independent of the size or mass of individual molecules.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Molecular Weight
Molecular weight, also known as molar mass, is the mass of one molecule of a substance calculated based on the sum of atomic weights of its constituent atoms. It is expressed in atomic mass units (amu) or grams per mole. When considering molar heat capacity, it’s crucial to understand that it represents a property per mole of substance. Since it measures the heat needed to increase the temperature of one mole, the individual mass of the molecules doesn’t affect this value.
This is why the molecular weight doesn’t influence the molar heat capacity. Rather than a focus on mass, molar heat capacity essentially regards the quantity of substance in moles, maintaining consistency despite variations in molecular weight.
Atomicity
Atomicity refers to the number of atoms present within a single molecule of a substance. This concept is significant when evaluating the molar heat capacity of gases. The number of atoms in a molecule, or its atomicity, impacts the degrees of freedom available for motion.
Each additional atom increases the potential energy modes, such as translational, rotational, and vibrational, which in turn alters the molar heat capacity. For example:
  • Monoatomic gases, like helium, have lower molar heat capacities as they primarily exhibit translational motion.
  • Diatomic or polyatomic gases have higher heat capacities due to additional rotational and vibrational degrees of freedom.
Hence, the atomicity directly influences how much energy a gas can absorb as heat.
Temperature Dependence
Temperature dependence refers to how a substance's physical property changes with temperature. When dealing with gases, their molar heat capacity can indeed vary with temperature. This variability is attributed to changes in the activity of molecules as they absorb more heat at higher temperatures.
At low temperatures, only a few degrees of freedom may be active. As temperature increases, additional rotational and vibrational motions become significant, amplifying heat capacity. Higher energy levels become accessible with rising temperatures, altering the total energy absorbed per mole. Understanding the temperature dependence of molar heat capacity helps predict how a gas will behave under different thermal conditions.
Conditions of Heat Supply
The conditions under which heat is supplied, such as constant pressure or constant volume, significantly impact the molar heat capacity of a gas. Molar heat capacity varies under different thermodynamic processes:
  • At constant volume ( C_v ), no work is done by expansion, and all supplied heat increases the internal energy.
  • At constant pressure ( C_p ), the gas expands as it is heated, performing work, requiring more energy per mole than at constant volume.
Additionally, specific processes like isothermal (constant temperature) or adiabatic (no heat exchange) conditions further modify how heat capacity is utilized. Each condition alters the energy requirements due to differences in how heat transforms into work or increases internal energy, thereby affecting calculations and applications of thermodynamic processes.

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Most popular questions from this chapter

Three rods cach of same length and cross section are joined in scrics. The thermal conductivity of the materials are \(k, 2 k\) and \(3 k\) respectively. If one end is kepl al \(200^{\circ} \mathrm{C}\) and the other at \(100^{\circ} \mathrm{C}\). What would be the temperature of the junctions in the steady state? \Lambdassume that no heat is lost duc to radiation from the sides of the rods.

\(\triangle 10 \mathrm{~kW}\) drilling machine is used to drill a bore in a small aluminium block of mass \(8.0 \mathrm{~kg}\). 1low much is the rise in temperature of the block in \(2.5\) minute? \(\Lambda\) ssuming \(50 \%\) of power is used up in heating the machine itself or lost the surroundings specific heat of aluminium \(=0.91 \mathrm{~J} / \mathrm{g}-{ }^{\circ} \mathrm{C}\)

Two bodies of same size \(P\) and \(Q\) are placed in a room which is maintained at a very low temperature. The bodies \(P\) and \(Q\) have temperatures \(527^{\circ} \mathrm{C}\) and \(127^{\circ} \mathrm{C}\) respectively. The energy radiated by \(P\) is (a) equal to \(Q\) (b) less than \(Q\) (c) greater than \(Q\) (d) 16 times greater than \(Q\)

The temperaturc of cqual masses of three differen liquids \(\Lambda, B\) and \(C\) are \(12^{\circ} \mathrm{C}\), \(19^{\circ} \mathrm{C}\) and \(28^{\circ} \mathrm{C}\). respectively. The temperature when \(A\) and \(B\) are mixed is \(16^{\circ} \mathrm{C}\) and when \(B\) and \(C\) are mixed it is \(23^{\circ} \mathrm{C}\). What should be the temperature when \(\Lambda\) and \(C\) are mixed?

Statement-1: Bodies radiate heat at all temperature. Statement-2: Rate of radiation of heat is proportional to the fourth power of absolute temperature.

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