400 m/s
200 m/s
800 m/s
200\(\sqrt{2}\) m/s
400\(\sqrt{2}\) m/s
Initial conditions: \[ v_{rms} = 200\,\text{m/s at temperature } T \text{ for diatomic gas} \]
RMS speed formula: \[ v_{rms} = \sqrt{\frac{3RT}{M}} \]
After changes:
New rms speed calculation: \[ v'_{rms} = \sqrt{\frac{3R(4T)}{M/2}} = \sqrt{8 \times \frac{3RT}{M}} \] \[ v'_{rms} = \sqrt{8} \times v_{rms} = 2\sqrt{2} \times 200 \] \[ v'_{rms} = 400\sqrt{2}\,\text{m/s} \]
Thus, the correct option (E) \(400\sqrt{2}\,\text{m/s}\).
1. Recall the formula for rms speed:
The root-mean-square (rms) speed (vrms) of gas molecules is given by:
\[v_{rms} = \sqrt{\frac{3kT}{m}} = \sqrt{\frac{3RT}{M}}\]
where:
2. Set up the initial and final conditions:
Initial conditions (diatomic, temperature T):
\[v_{rms1} = \sqrt{\frac{3kT}{m_1}} = 200 \, m/s\]
Final conditions (monoatomic, temperature 4T, mass is halved since molecules dissociate):
\[v_{rms2} = \sqrt{\frac{3k(4T)}{m_2}}\] Since the diatomic molecules dissociate into monoatomic atoms, the mass of each atom is half the mass of the diatomic molecule: \(m_2 = \frac{m_1}{2}\). \[v_{rms2} = \sqrt{\frac{3k(4T)}{m_1/2}} = \sqrt{8 \frac{3kT}{m_1}} \]
3. Relate the final rms speed to the initial rms speed:
\[v_{rms2} = \sqrt{8} \sqrt{\frac{3kT}{m_1}} = 2\sqrt{2} v_{rms1} \]
Since \(v_{rms1} = 200 \, m/s\):
\[v_{rms2} = 2\sqrt{2}(200 \, m/s) = 400\sqrt{2} \, m/s\]
Final Answer: The final answer is \(\boxed{E}\)
Consider a rope fixed at both ends under tension so that it is horizontal (i.e. assume the rope is along x-axis, with gravity acting along z-axis). Now the right end is continually oscillated at high frequency n (say n=100 Hz) horizontally and in a direction along the rope; amplitude of oscillation is negligible. The oscillation travells along the rope and is reflected at the left end.
Let the total length of rope be l, total mass be m and the acceleration due to gravity be g.
After initial phase (say a mintue or so), the rope has __(BLANK-1)__ wave, which is __(BLANK-2)__ in nature. It results from superposition of left travelling and right travelling __(BLANK-3)__ waves. This resulting wave has a frequency __ (BLANK-4)_ that of oscillation frequency nu. Simple dimensional analysis indicates that the frequency of can be of the form: ___(BLANK-5)__ .
If \( 2 \) is a solution of the inequality \( \frac{x-a}{a-2x}<-3 \), then \( a \) must lie in the interval:
Real gases are gases that do not follow the ideal gas law, which assumes that gas particles have negligible volume and no intermolecular forces. In reality, gas particles do have volume and interact with each other, leading to deviations from ideal gas behavior.
The behavior of real gases can be described using various gas laws, such as the van der Waals equation and the virial equation. These equations take into account the effects of gas particle size and intermolecular forces on gas behavior.
One important property of real gases is compressibility. Real gases are more compressible than ideal gases, meaning that they can be compressed to a smaller volume at the same pressure. This is due to the fact that gas particles occupy a finite amount of space and are subject to intermolecular forces that can cause them to come closer together.
Also Read: Derivation from Ideal Gas Behavior
Another property of real gases is that their behavior is strongly affected by temperature and pressure. At high pressures and low temperatures, real gases tend to deviate more from ideal gas behavior. This is because the intermolecular forces become stronger and the gas particles are closer together.
Real gases also exhibit a phenomenon called condensation, where gas particles condense into a liquid or solid state when cooled or compressed sufficiently. This is due to the fact that the intermolecular forces become strong enough to overcome the kinetic energy of the gas particles, causing them to condense into a denser state.
Overall, the behavior of real gases is complex and influenced by various factors such as temperature, pressure, and intermolecular forces. Understanding the behavior of real gases is important in many scientific and industrial applications, such as in chemical reactions, power generation, and refrigeration.