In the given \({(V\text{-}T)}\) diagram, what is the relation between pressure \({P_1}\) and \({P_2}\)? 

1. \(P_2>P_1\) 2. \(P_2<P_1\)
3. cannot be predicted 4. \(P_2=P_1\)

Subtopic:  Ideal Gas Equation |
 84%
Level 1: 80%+
AIPMT - 2013
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The molar specific heats of an ideal gas at constant pressure and volume are denoted by \(C_P\) and \(C_V,\) respectively. If \(\gamma =\frac{C_P}{C_V}\) and \(R\) is the universal gas constant, then \(C_V\) is equal to:
1. \(\dfrac{R}{\gamma -1}\) 2. \(\dfrac{\gamma -1}{R}\)
3. \(\gamma R \) 4. \(\dfrac{\left ( \gamma -1 \right )R}{\left ( \gamma +1 \right )}\)
Subtopic:  Molar Specific Heat |
 89%
Level 1: 80%+
AIPMT - 2013
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The amount of heat energy required to raise the temperature of \(1\) g of Helium at NTP, from \({T_1}\) K to \({T_2}\) K is:

1. \(\dfrac{3}{2}N_ak_B(T_2-T_1)\) 2. \(\dfrac{3}{4}N_ak_B(T_2-T_1)\)
3. \(\dfrac{3}{4}N_ak_B\frac{T_2}{T_1}\) 4. \(\dfrac{3}{8}N_ak_B(T_2-T_1)\)
Subtopic:  Specific Heat |
 53%
Level 3: 35%-60%
AIPMT - 2013
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A plano-convex lens fits exactly into a plano-concave lens. Their plane surfaces are parallel to each other. If lenses are made of different materials of refractive indices \(\mu_1\) and \(\mu_2\) and \(R\) is the radius of curvature of the curved surface of the lenses, then the focal length of the combination is:
1. \(\dfrac{R}{2(\mu_1-\mu_2)}\) 2. \(\dfrac{R}{(\mu_1-\mu_2)}\)
3. \(\dfrac{2R}{(\mu_2-\mu_1)}\) 4. \(\dfrac{R}{2(\mu_1+\mu_2)}\)
Subtopic:  Lens Makers' Formula |
 69%
Level 2: 60%+
AIPMT - 2013
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During an adiabatic process, the pressure of a gas is found to be proportional to the cube of its temperature. The ratio of \(\frac{C_P}{C_V}\) for the gas is:
1. \(2\)
2. \(5/3\)
3. \(3/2\)
4. \(4/3\)
Subtopic:  Types of Processes |
 71%
Level 2: 60%+
AIPMT - 2013
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A wave traveling in the +ve \(x\text-\)direction having maximum displacement along \(y\text-\)direction as \(1~\text{m}\), wavelength \(2\pi~\text{m}\) and frequency of \(\frac{1}{\pi}~\text{Hz}\), is represented by:

1. \(y=\sin (2 \pi x-2 \pi t)\) 2. \(y=\sin (10 \pi x-20 \pi t)\)
3. \(y=\sin (2 \pi x+2 \pi t)\) 4. \( y=\sin (x-2 t)\)
Subtopic:  Wave Motion |
 88%
Level 1: 80%+
AIPMT - 2013
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The output \((X)\) of the logic circuit shown in the figure will be: 
  
1. \(X= \overline{A\cdot B}\)
2. \(X = A\cdot B\)
3. \(X= \overline{A+ B}\)
4. None of the above

Subtopic:  Logic gates |
 79%
Level 2: 60%+
AIPMT - 2013
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A body of mass \(m\) is taken from the Earth’s surface to the height equal to twice the radius \((R)\) of the Earth. The change in potential energy of the body will be: 

1. \(\frac{2}{3}mgR\) 2. \(3mgR\)
3. \(\frac{1}{3}mgR\) 4. \(2mgR\)
Subtopic:  Gravitational Potential Energy |
 78%
Level 2: 60%+
AIPMT - 2013
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The ratio of the longest wavelengths corresponding to the Lyman and Balmer series in the hydrogen spectrum is:
1. \(\dfrac{3}{23}\) 2. \(\dfrac{7}{29}\)
3. \(\dfrac{9}{31}\) 4. \(\dfrac{5}{27}\)
Subtopic:  Spectral Series |
 89%
Level 1: 80%+
AIPMT - 2013
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An infinite number of bodies, each of mass \(2~\text{kg}\) are situated on the \(x\text-\)axis at distances \(1 ~\text m, ~2~\text m, ~4~\text m, ~8~\text m,......\)respectively, from the origin. The resulting gravitational potential due to this system at the origin will be:
1.  \(-\dfrac{8}{3}{G}\) 2. \(-\dfrac{4}{3} {G}\)
3.  \(-4 {G}\) 4. \(-{G}\)
Subtopic:  Gravitational Potential |
 70%
Level 2: 60%+
AIPMT - 2013
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