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chhitiz
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how does specific heat of gases vary with temperature? is there an equation to describe it?
chhitiz said:how does specific heat of gases vary with temperature? is there an equation to describe it?
stewartcs said:In Thermodynamics specific heats are defined as:
[tex]C_v = \Bigg(\frac{\partial{u}}{\partial{T}}\Bigg)_v [/tex]
[tex]C_p = \Bigg(\frac{\partial{h}}{\partial{T}}\Bigg)_p [/tex]
So yes, they are temperature dependent.
CS
stewartcs said:In Thermodynamics specific heats are defined as:
So yes, they are temperature dependent.
CS
Mapes said:(I must point out that the second statement doesn't follow from the definitions; if [itex]U\propto T[/itex], for example, then [itex]c_V[/itex] would be constant. And this is approximately the case for common gases at common pressures, where [itex]c_V[/itex] is an essentially constant 3R/2 or 5R/2 for monatomic and diatomic gases, respectively.)
Topher925 said:This doesn't really state that heat capacity is dependent upon temperature though. It actually states that internal energy or enthalpy is dependent upon temperature, not heat capacity.
Topher925 said:Theoretically, the heat capacity of a gas should not change with temperature and should only depend on its molecular composition. In reality, this isn't the case and heat capacities must be determined experimentally at different temperatures. You won't find a single use-all equation for heat capacity of different gases. Instead, empirical correlations are used which are determined using experimental data and curve fits.
stewartcs said:For a diatomic gas at a certain range of temperatures the only mode excited is the translational mode. As the temperature increases and more KE is added, the rotational mode is excited (and the KE will now be stored there as well). If the temperature is increase yet again and even more KE is added to the gas, the vibrational mode will be excited and the KE stored there as well.
The result is that the commonly quoted value of 5R/2 for a diatomic molecule is only for the translational mode. The other modes are essentially dormant or frozen out until enough KE has been added to excite them.
The value becomes 7R/2 when the temperature increases enough to excite the rotational mode, and then 9R/2 when the temperature increases enough to excite the vibrational mode.
Mapes said:Agreed, but please note what temperature these transitions typically occur: for nitrogen between ~100-2000K, for example, the translational and rotational modes (but not the vibrational mode) are excited, the energy [itex]U\propto T[/itex] (specifically, [itex]U\approx 5NRT/2[/itex]), and the constant-volume specific heat is an approximately constant 5R/2. That's what I meant when I wrote "common gases at common [temperatures]."
Specific heat is the amount of heat required to raise the temperature of a substance by one degree. It varies with temperature because as the temperature increases, the particles in the substance have more kinetic energy and are able to absorb more heat without a significant increase in temperature.
The relationship between specific heat and temperature is inverse. As temperature increases, specific heat decreases. This means that it takes less heat to raise the temperature of a substance at higher temperatures compared to lower temperatures.
The variation of specific heat with temperature affects heat transfer by influencing how much heat is needed to raise the temperature of a substance. As specific heat decreases with increasing temperature, less heat is required for the substance to reach a higher temperature. This can impact the efficiency of heat transfer processes.
The variation of specific heat with temperature can be affected by factors such as the molecular structure of the substance, the type of bonding between molecules, and the presence of impurities or other substances in the material.
The variation of specific heat with temperature is typically measured using calorimetry, which involves measuring the change in temperature of a substance when a known amount of heat is added or removed. The specific heat can then be calculated using the formula Q = mCΔT, where Q is the heat added or removed, m is the mass of the substance, C is the specific heat, and ΔT is the change in temperature.