FST 3
TEST SERIES (PHYSICS FST)

266230 At what temperature the r.m.s velocity of a hydrogen molecule is equal to that of an oxygen molecule at \(27^{\circ} \mathrm{C}\) :

1 80 K
2 -73 K
3 18.75 K
4 20 K
TEST SERIES (PHYSICS FST)

266231 A simple pendulum executing S.H.M. about \(x=0\) with period T and amplitude A . Its speed when at a distance \(\frac{A}{3}\) from its mean position:

1 \(\frac{\pi A \sqrt{3}}{T}\)
2 \(\frac{\pi \mathrm{A} \sqrt{15}}{\mathrm{~T}}\)
3 \(\frac{\pi \mathrm{A}}{2 \mathrm{~T}}\)
4 \(\frac{4 \pi A \sqrt{2}}{3 T}\)
TEST SERIES (PHYSICS FST)

266232 In a thermodynamic process, pressure of a fixed mass of an ideal gas is changed in such a manner that the gas molecules gives out 20 J of heat and 8 J of work is done on the gas. If the initial internal energy of the gas was 30 J . then the final internal energy will be:

1 30 J
2 18 J
3 22 J
4 40 J
TEST SERIES (PHYSICS FST)

266233 A charged particle is balanced in an electric field E If direction of field is reversed then find net force on particle:

1 mg
2 3 mg
3 2 mg
4 Zero.
TEST SERIES (PHYSICS FST)

266234 A point electric dipole \(\overrightarrow{\mathrm{p}}=-\mathrm{P}_0 \hat{\mathrm{x}}\) is kept at the origin. The potential and electric field due to this dipole on the \(y\)-axis at a distance \(d\) are respectively: (Take V = 0 at infinity):

1 \(\frac{|\vec{p}|}{4 \pi \varepsilon_0 d^2} \cdot \frac{-\vec{p}}{4 \pi \varepsilon_0 d^3}\)
2 \(0, \frac{\overrightarrow{\mathrm{P}}}{4 \pi \varepsilon_0 \mathrm{~d}^3}\)
3 \(\frac{|\vec{p}|}{4 \pi \varepsilon_0 \mathrm{~d}^2}, \frac{\vec{p}}{4 \pi \varepsilon_0 \mathrm{~d}^3}\)
4 \(0, \frac{-\vec{p}}{4 \pi \varepsilon_0 d^3}\)
TEST SERIES (PHYSICS FST)

266230 At what temperature the r.m.s velocity of a hydrogen molecule is equal to that of an oxygen molecule at \(27^{\circ} \mathrm{C}\) :

1 80 K
2 -73 K
3 18.75 K
4 20 K
TEST SERIES (PHYSICS FST)

266231 A simple pendulum executing S.H.M. about \(x=0\) with period T and amplitude A . Its speed when at a distance \(\frac{A}{3}\) from its mean position:

1 \(\frac{\pi A \sqrt{3}}{T}\)
2 \(\frac{\pi \mathrm{A} \sqrt{15}}{\mathrm{~T}}\)
3 \(\frac{\pi \mathrm{A}}{2 \mathrm{~T}}\)
4 \(\frac{4 \pi A \sqrt{2}}{3 T}\)
TEST SERIES (PHYSICS FST)

266232 In a thermodynamic process, pressure of a fixed mass of an ideal gas is changed in such a manner that the gas molecules gives out 20 J of heat and 8 J of work is done on the gas. If the initial internal energy of the gas was 30 J . then the final internal energy will be:

1 30 J
2 18 J
3 22 J
4 40 J
TEST SERIES (PHYSICS FST)

266233 A charged particle is balanced in an electric field E If direction of field is reversed then find net force on particle:

1 mg
2 3 mg
3 2 mg
4 Zero.
TEST SERIES (PHYSICS FST)

266234 A point electric dipole \(\overrightarrow{\mathrm{p}}=-\mathrm{P}_0 \hat{\mathrm{x}}\) is kept at the origin. The potential and electric field due to this dipole on the \(y\)-axis at a distance \(d\) are respectively: (Take V = 0 at infinity):

1 \(\frac{|\vec{p}|}{4 \pi \varepsilon_0 d^2} \cdot \frac{-\vec{p}}{4 \pi \varepsilon_0 d^3}\)
2 \(0, \frac{\overrightarrow{\mathrm{P}}}{4 \pi \varepsilon_0 \mathrm{~d}^3}\)
3 \(\frac{|\vec{p}|}{4 \pi \varepsilon_0 \mathrm{~d}^2}, \frac{\vec{p}}{4 \pi \varepsilon_0 \mathrm{~d}^3}\)
4 \(0, \frac{-\vec{p}}{4 \pi \varepsilon_0 d^3}\)
TEST SERIES (PHYSICS FST)

266230 At what temperature the r.m.s velocity of a hydrogen molecule is equal to that of an oxygen molecule at \(27^{\circ} \mathrm{C}\) :

1 80 K
2 -73 K
3 18.75 K
4 20 K
TEST SERIES (PHYSICS FST)

266231 A simple pendulum executing S.H.M. about \(x=0\) with period T and amplitude A . Its speed when at a distance \(\frac{A}{3}\) from its mean position:

1 \(\frac{\pi A \sqrt{3}}{T}\)
2 \(\frac{\pi \mathrm{A} \sqrt{15}}{\mathrm{~T}}\)
3 \(\frac{\pi \mathrm{A}}{2 \mathrm{~T}}\)
4 \(\frac{4 \pi A \sqrt{2}}{3 T}\)
TEST SERIES (PHYSICS FST)

266232 In a thermodynamic process, pressure of a fixed mass of an ideal gas is changed in such a manner that the gas molecules gives out 20 J of heat and 8 J of work is done on the gas. If the initial internal energy of the gas was 30 J . then the final internal energy will be:

1 30 J
2 18 J
3 22 J
4 40 J
TEST SERIES (PHYSICS FST)

266233 A charged particle is balanced in an electric field E If direction of field is reversed then find net force on particle:

1 mg
2 3 mg
3 2 mg
4 Zero.
TEST SERIES (PHYSICS FST)

266234 A point electric dipole \(\overrightarrow{\mathrm{p}}=-\mathrm{P}_0 \hat{\mathrm{x}}\) is kept at the origin. The potential and electric field due to this dipole on the \(y\)-axis at a distance \(d\) are respectively: (Take V = 0 at infinity):

1 \(\frac{|\vec{p}|}{4 \pi \varepsilon_0 d^2} \cdot \frac{-\vec{p}}{4 \pi \varepsilon_0 d^3}\)
2 \(0, \frac{\overrightarrow{\mathrm{P}}}{4 \pi \varepsilon_0 \mathrm{~d}^3}\)
3 \(\frac{|\vec{p}|}{4 \pi \varepsilon_0 \mathrm{~d}^2}, \frac{\vec{p}}{4 \pi \varepsilon_0 \mathrm{~d}^3}\)
4 \(0, \frac{-\vec{p}}{4 \pi \varepsilon_0 d^3}\)
TEST SERIES (PHYSICS FST)

266230 At what temperature the r.m.s velocity of a hydrogen molecule is equal to that of an oxygen molecule at \(27^{\circ} \mathrm{C}\) :

1 80 K
2 -73 K
3 18.75 K
4 20 K
TEST SERIES (PHYSICS FST)

266231 A simple pendulum executing S.H.M. about \(x=0\) with period T and amplitude A . Its speed when at a distance \(\frac{A}{3}\) from its mean position:

1 \(\frac{\pi A \sqrt{3}}{T}\)
2 \(\frac{\pi \mathrm{A} \sqrt{15}}{\mathrm{~T}}\)
3 \(\frac{\pi \mathrm{A}}{2 \mathrm{~T}}\)
4 \(\frac{4 \pi A \sqrt{2}}{3 T}\)
TEST SERIES (PHYSICS FST)

266232 In a thermodynamic process, pressure of a fixed mass of an ideal gas is changed in such a manner that the gas molecules gives out 20 J of heat and 8 J of work is done on the gas. If the initial internal energy of the gas was 30 J . then the final internal energy will be:

1 30 J
2 18 J
3 22 J
4 40 J
TEST SERIES (PHYSICS FST)

266233 A charged particle is balanced in an electric field E If direction of field is reversed then find net force on particle:

1 mg
2 3 mg
3 2 mg
4 Zero.
TEST SERIES (PHYSICS FST)

266234 A point electric dipole \(\overrightarrow{\mathrm{p}}=-\mathrm{P}_0 \hat{\mathrm{x}}\) is kept at the origin. The potential and electric field due to this dipole on the \(y\)-axis at a distance \(d\) are respectively: (Take V = 0 at infinity):

1 \(\frac{|\vec{p}|}{4 \pi \varepsilon_0 d^2} \cdot \frac{-\vec{p}}{4 \pi \varepsilon_0 d^3}\)
2 \(0, \frac{\overrightarrow{\mathrm{P}}}{4 \pi \varepsilon_0 \mathrm{~d}^3}\)
3 \(\frac{|\vec{p}|}{4 \pi \varepsilon_0 \mathrm{~d}^2}, \frac{\vec{p}}{4 \pi \varepsilon_0 \mathrm{~d}^3}\)
4 \(0, \frac{-\vec{p}}{4 \pi \varepsilon_0 d^3}\)
TEST SERIES (PHYSICS FST)

266230 At what temperature the r.m.s velocity of a hydrogen molecule is equal to that of an oxygen molecule at \(27^{\circ} \mathrm{C}\) :

1 80 K
2 -73 K
3 18.75 K
4 20 K
TEST SERIES (PHYSICS FST)

266231 A simple pendulum executing S.H.M. about \(x=0\) with period T and amplitude A . Its speed when at a distance \(\frac{A}{3}\) from its mean position:

1 \(\frac{\pi A \sqrt{3}}{T}\)
2 \(\frac{\pi \mathrm{A} \sqrt{15}}{\mathrm{~T}}\)
3 \(\frac{\pi \mathrm{A}}{2 \mathrm{~T}}\)
4 \(\frac{4 \pi A \sqrt{2}}{3 T}\)
TEST SERIES (PHYSICS FST)

266232 In a thermodynamic process, pressure of a fixed mass of an ideal gas is changed in such a manner that the gas molecules gives out 20 J of heat and 8 J of work is done on the gas. If the initial internal energy of the gas was 30 J . then the final internal energy will be:

1 30 J
2 18 J
3 22 J
4 40 J
TEST SERIES (PHYSICS FST)

266233 A charged particle is balanced in an electric field E If direction of field is reversed then find net force on particle:

1 mg
2 3 mg
3 2 mg
4 Zero.
TEST SERIES (PHYSICS FST)

266234 A point electric dipole \(\overrightarrow{\mathrm{p}}=-\mathrm{P}_0 \hat{\mathrm{x}}\) is kept at the origin. The potential and electric field due to this dipole on the \(y\)-axis at a distance \(d\) are respectively: (Take V = 0 at infinity):

1 \(\frac{|\vec{p}|}{4 \pi \varepsilon_0 d^2} \cdot \frac{-\vec{p}}{4 \pi \varepsilon_0 d^3}\)
2 \(0, \frac{\overrightarrow{\mathrm{P}}}{4 \pi \varepsilon_0 \mathrm{~d}^3}\)
3 \(\frac{|\vec{p}|}{4 \pi \varepsilon_0 \mathrm{~d}^2}, \frac{\vec{p}}{4 \pi \varepsilon_0 \mathrm{~d}^3}\)
4 \(0, \frac{-\vec{p}}{4 \pi \varepsilon_0 d^3}\)