Gravitational Potential
PHXI08:GRAVITATION

359875 \(P(r)\) is magnitude of physical quantity as a function of \(r\) (distance from centre of spherical distribution of radius \(R\) ). Match the following columns and select the correct option from the codes given below:
supporting img

1 \(\mathrm{A}-\mathrm{S}, \mathrm{B}-\mathrm{R}, \mathrm{C}-\mathrm{Q}, \mathrm{D}-\mathrm{P}\)
2 \(\mathrm{A}-\mathrm{Q}, \mathrm{B}-\mathrm{S}, \mathrm{C}-\mathrm{R}, \mathrm{D}-\mathrm{P}\)
3 \(\mathrm{A}-\mathrm{Q}, \mathrm{B}-\mathrm{R}, \mathrm{C}-\mathrm{S}, \mathrm{D}-\mathrm{P}\)
4 \(\mathrm{A}-\mathrm{R}, \mathrm{B}-\mathrm{S}, \mathrm{C}-\mathrm{P}, \mathrm{D}-\mathrm{Q}\)
PHXI08:GRAVITATION

359876 The gravitational potential at a point above the surface of earth is \( - 5.12 \times {10^7}\;J/kg\) and the acceleration due to gravity at that point is \(6.4\;m/{s^2}.\) Assume that the mean radius of earth to be \(6400\,km\) . The height of this point above the earth's surface is

1 \(1600\,km\)
2 \(540\,km\)
3 \(1200\,km\)
4 \(1000\,km\)
PHXI08:GRAVITATION

359877 Two rings having masses \(M\) and \(2 M\), respectively, having same radius are placed coaxially as shown in figure. If the mass distribution on both the rings is non-uniform, then gravitational potential at point \(P\) is
supporting img

1 \(-\dfrac{G M}{R}\left[\dfrac{1}{\sqrt{2}}+\dfrac{2}{\sqrt{5}}\right]\)
2 \(-\dfrac{G M}{R}\left[1+\dfrac{2}{2}\right]\)
3 Zero
4 Cannot be determined from given information.
PHXI08:GRAVITATION

359878 Two hollow spherical shells each of mass \(m\) and radii \(R\) and \(2R\) are present. The potential at the centre is

1 \(\dfrac{-G m}{2 R}\)
2 \(\dfrac{-3 G m}{2 R}\)
3 \(\dfrac{-G m}{R}\)
4 \(\dfrac{-G m}{3 R}\)
PHXI08:GRAVITATION

359879 For a uniform ring of mass \(M\) and radius \(R\) at its centre

1 Field and potential both are zero
2 Field is zero but potential is \(\dfrac{G M}{R}\)
3 Field is zero but potential is \( - GM/R\)
4 Magnitude of field is \(\frac{{GM}}{{{R^2}}}\) and potential is \( - \frac{{GM}}{R}\)
PHXI08:GRAVITATION

359875 \(P(r)\) is magnitude of physical quantity as a function of \(r\) (distance from centre of spherical distribution of radius \(R\) ). Match the following columns and select the correct option from the codes given below:
supporting img

1 \(\mathrm{A}-\mathrm{S}, \mathrm{B}-\mathrm{R}, \mathrm{C}-\mathrm{Q}, \mathrm{D}-\mathrm{P}\)
2 \(\mathrm{A}-\mathrm{Q}, \mathrm{B}-\mathrm{S}, \mathrm{C}-\mathrm{R}, \mathrm{D}-\mathrm{P}\)
3 \(\mathrm{A}-\mathrm{Q}, \mathrm{B}-\mathrm{R}, \mathrm{C}-\mathrm{S}, \mathrm{D}-\mathrm{P}\)
4 \(\mathrm{A}-\mathrm{R}, \mathrm{B}-\mathrm{S}, \mathrm{C}-\mathrm{P}, \mathrm{D}-\mathrm{Q}\)
PHXI08:GRAVITATION

359876 The gravitational potential at a point above the surface of earth is \( - 5.12 \times {10^7}\;J/kg\) and the acceleration due to gravity at that point is \(6.4\;m/{s^2}.\) Assume that the mean radius of earth to be \(6400\,km\) . The height of this point above the earth's surface is

1 \(1600\,km\)
2 \(540\,km\)
3 \(1200\,km\)
4 \(1000\,km\)
PHXI08:GRAVITATION

359877 Two rings having masses \(M\) and \(2 M\), respectively, having same radius are placed coaxially as shown in figure. If the mass distribution on both the rings is non-uniform, then gravitational potential at point \(P\) is
supporting img

1 \(-\dfrac{G M}{R}\left[\dfrac{1}{\sqrt{2}}+\dfrac{2}{\sqrt{5}}\right]\)
2 \(-\dfrac{G M}{R}\left[1+\dfrac{2}{2}\right]\)
3 Zero
4 Cannot be determined from given information.
PHXI08:GRAVITATION

359878 Two hollow spherical shells each of mass \(m\) and radii \(R\) and \(2R\) are present. The potential at the centre is

1 \(\dfrac{-G m}{2 R}\)
2 \(\dfrac{-3 G m}{2 R}\)
3 \(\dfrac{-G m}{R}\)
4 \(\dfrac{-G m}{3 R}\)
PHXI08:GRAVITATION

359879 For a uniform ring of mass \(M\) and radius \(R\) at its centre

1 Field and potential both are zero
2 Field is zero but potential is \(\dfrac{G M}{R}\)
3 Field is zero but potential is \( - GM/R\)
4 Magnitude of field is \(\frac{{GM}}{{{R^2}}}\) and potential is \( - \frac{{GM}}{R}\)
NEET Test Series from KOTA - 10 Papers In MS WORD WhatsApp Here
PHXI08:GRAVITATION

359875 \(P(r)\) is magnitude of physical quantity as a function of \(r\) (distance from centre of spherical distribution of radius \(R\) ). Match the following columns and select the correct option from the codes given below:
supporting img

1 \(\mathrm{A}-\mathrm{S}, \mathrm{B}-\mathrm{R}, \mathrm{C}-\mathrm{Q}, \mathrm{D}-\mathrm{P}\)
2 \(\mathrm{A}-\mathrm{Q}, \mathrm{B}-\mathrm{S}, \mathrm{C}-\mathrm{R}, \mathrm{D}-\mathrm{P}\)
3 \(\mathrm{A}-\mathrm{Q}, \mathrm{B}-\mathrm{R}, \mathrm{C}-\mathrm{S}, \mathrm{D}-\mathrm{P}\)
4 \(\mathrm{A}-\mathrm{R}, \mathrm{B}-\mathrm{S}, \mathrm{C}-\mathrm{P}, \mathrm{D}-\mathrm{Q}\)
PHXI08:GRAVITATION

359876 The gravitational potential at a point above the surface of earth is \( - 5.12 \times {10^7}\;J/kg\) and the acceleration due to gravity at that point is \(6.4\;m/{s^2}.\) Assume that the mean radius of earth to be \(6400\,km\) . The height of this point above the earth's surface is

1 \(1600\,km\)
2 \(540\,km\)
3 \(1200\,km\)
4 \(1000\,km\)
PHXI08:GRAVITATION

359877 Two rings having masses \(M\) and \(2 M\), respectively, having same radius are placed coaxially as shown in figure. If the mass distribution on both the rings is non-uniform, then gravitational potential at point \(P\) is
supporting img

1 \(-\dfrac{G M}{R}\left[\dfrac{1}{\sqrt{2}}+\dfrac{2}{\sqrt{5}}\right]\)
2 \(-\dfrac{G M}{R}\left[1+\dfrac{2}{2}\right]\)
3 Zero
4 Cannot be determined from given information.
PHXI08:GRAVITATION

359878 Two hollow spherical shells each of mass \(m\) and radii \(R\) and \(2R\) are present. The potential at the centre is

1 \(\dfrac{-G m}{2 R}\)
2 \(\dfrac{-3 G m}{2 R}\)
3 \(\dfrac{-G m}{R}\)
4 \(\dfrac{-G m}{3 R}\)
PHXI08:GRAVITATION

359879 For a uniform ring of mass \(M\) and radius \(R\) at its centre

1 Field and potential both are zero
2 Field is zero but potential is \(\dfrac{G M}{R}\)
3 Field is zero but potential is \( - GM/R\)
4 Magnitude of field is \(\frac{{GM}}{{{R^2}}}\) and potential is \( - \frac{{GM}}{R}\)
PHXI08:GRAVITATION

359875 \(P(r)\) is magnitude of physical quantity as a function of \(r\) (distance from centre of spherical distribution of radius \(R\) ). Match the following columns and select the correct option from the codes given below:
supporting img

1 \(\mathrm{A}-\mathrm{S}, \mathrm{B}-\mathrm{R}, \mathrm{C}-\mathrm{Q}, \mathrm{D}-\mathrm{P}\)
2 \(\mathrm{A}-\mathrm{Q}, \mathrm{B}-\mathrm{S}, \mathrm{C}-\mathrm{R}, \mathrm{D}-\mathrm{P}\)
3 \(\mathrm{A}-\mathrm{Q}, \mathrm{B}-\mathrm{R}, \mathrm{C}-\mathrm{S}, \mathrm{D}-\mathrm{P}\)
4 \(\mathrm{A}-\mathrm{R}, \mathrm{B}-\mathrm{S}, \mathrm{C}-\mathrm{P}, \mathrm{D}-\mathrm{Q}\)
PHXI08:GRAVITATION

359876 The gravitational potential at a point above the surface of earth is \( - 5.12 \times {10^7}\;J/kg\) and the acceleration due to gravity at that point is \(6.4\;m/{s^2}.\) Assume that the mean radius of earth to be \(6400\,km\) . The height of this point above the earth's surface is

1 \(1600\,km\)
2 \(540\,km\)
3 \(1200\,km\)
4 \(1000\,km\)
PHXI08:GRAVITATION

359877 Two rings having masses \(M\) and \(2 M\), respectively, having same radius are placed coaxially as shown in figure. If the mass distribution on both the rings is non-uniform, then gravitational potential at point \(P\) is
supporting img

1 \(-\dfrac{G M}{R}\left[\dfrac{1}{\sqrt{2}}+\dfrac{2}{\sqrt{5}}\right]\)
2 \(-\dfrac{G M}{R}\left[1+\dfrac{2}{2}\right]\)
3 Zero
4 Cannot be determined from given information.
PHXI08:GRAVITATION

359878 Two hollow spherical shells each of mass \(m\) and radii \(R\) and \(2R\) are present. The potential at the centre is

1 \(\dfrac{-G m}{2 R}\)
2 \(\dfrac{-3 G m}{2 R}\)
3 \(\dfrac{-G m}{R}\)
4 \(\dfrac{-G m}{3 R}\)
PHXI08:GRAVITATION

359879 For a uniform ring of mass \(M\) and radius \(R\) at its centre

1 Field and potential both are zero
2 Field is zero but potential is \(\dfrac{G M}{R}\)
3 Field is zero but potential is \( - GM/R\)
4 Magnitude of field is \(\frac{{GM}}{{{R^2}}}\) and potential is \( - \frac{{GM}}{R}\)
PHXI08:GRAVITATION

359875 \(P(r)\) is magnitude of physical quantity as a function of \(r\) (distance from centre of spherical distribution of radius \(R\) ). Match the following columns and select the correct option from the codes given below:
supporting img

1 \(\mathrm{A}-\mathrm{S}, \mathrm{B}-\mathrm{R}, \mathrm{C}-\mathrm{Q}, \mathrm{D}-\mathrm{P}\)
2 \(\mathrm{A}-\mathrm{Q}, \mathrm{B}-\mathrm{S}, \mathrm{C}-\mathrm{R}, \mathrm{D}-\mathrm{P}\)
3 \(\mathrm{A}-\mathrm{Q}, \mathrm{B}-\mathrm{R}, \mathrm{C}-\mathrm{S}, \mathrm{D}-\mathrm{P}\)
4 \(\mathrm{A}-\mathrm{R}, \mathrm{B}-\mathrm{S}, \mathrm{C}-\mathrm{P}, \mathrm{D}-\mathrm{Q}\)
PHXI08:GRAVITATION

359876 The gravitational potential at a point above the surface of earth is \( - 5.12 \times {10^7}\;J/kg\) and the acceleration due to gravity at that point is \(6.4\;m/{s^2}.\) Assume that the mean radius of earth to be \(6400\,km\) . The height of this point above the earth's surface is

1 \(1600\,km\)
2 \(540\,km\)
3 \(1200\,km\)
4 \(1000\,km\)
PHXI08:GRAVITATION

359877 Two rings having masses \(M\) and \(2 M\), respectively, having same radius are placed coaxially as shown in figure. If the mass distribution on both the rings is non-uniform, then gravitational potential at point \(P\) is
supporting img

1 \(-\dfrac{G M}{R}\left[\dfrac{1}{\sqrt{2}}+\dfrac{2}{\sqrt{5}}\right]\)
2 \(-\dfrac{G M}{R}\left[1+\dfrac{2}{2}\right]\)
3 Zero
4 Cannot be determined from given information.
PHXI08:GRAVITATION

359878 Two hollow spherical shells each of mass \(m\) and radii \(R\) and \(2R\) are present. The potential at the centre is

1 \(\dfrac{-G m}{2 R}\)
2 \(\dfrac{-3 G m}{2 R}\)
3 \(\dfrac{-G m}{R}\)
4 \(\dfrac{-G m}{3 R}\)
PHXI08:GRAVITATION

359879 For a uniform ring of mass \(M\) and radius \(R\) at its centre

1 Field and potential both are zero
2 Field is zero but potential is \(\dfrac{G M}{R}\)
3 Field is zero but potential is \( - GM/R\)
4 Magnitude of field is \(\frac{{GM}}{{{R^2}}}\) and potential is \( - \frac{{GM}}{R}\)