Gravitational potential energy (general form) Knowledge-Based Practice

Physics · Forces & Newton's Laws · Physics · Circular Motion & Gravitation

10 Physics practice questions on Gravitational potential energy (general form). Questions that assess core concepts and understanding.

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Questions

  1. 1.

    An object of mass mm is moved radially away from the center of a planet of mass MM. If ΔU1\Delta U_1 is the change in gravitational potential energy when moving from radial distance rr to 2r2r, and ΔU2\Delta U_2 is the change when moving from 2r2r to 3r3r, what is the ratio ΔU1ΔU2\frac{\Delta U_1}{\Delta U_2}?

    • A) 3
    • B) 1
    • C) 2
    • D) 32\frac{3}{2}
  2. 2.

    If the zero-reference point for gravitational potential energy is chosen to be at the surface of a spherical planet of mass MM and radius RR, which expression gives the gravitational potential energy U(r)U(r) of an object of mass mm at a radial distance r≥Rr \ge R from the center of the planet?

    • A) U(r)=−GMm(1R−1r)U(r) = -GMm\left(\frac{1}{R} - \frac{1}{r}\right)
    • B) U(r)=−GMmr−RU(r) = -\frac{GMm}{r - R}
    • C) U(r)=GMm(1r−1R)U(r) = GMm\left(\frac{1}{r} - \frac{1}{R}\right)
    • D) U(r)=GMm(1R−1r)U(r) = GMm\left(\frac{1}{R} - \frac{1}{r}\right)
  3. 3.

    Which of the following expressions represents the work done by the gravitational force on an object of mass mm as it moves radially from an initial distance r1r_1 to a final distance r2r_2 from the center of a spherical planet of mass MM?

    • A) W=GMm(1r1−1r2)W = GMm\left(\frac{1}{r_1} - \frac{1}{r_2}\right)
    • B) W=GMm(1r12−1r22)W = GMm\left(\frac{1}{r_1^2} - \frac{1}{r_2^2}\right)
    • C) W=GMm(1r2−1r1)W = GMm\left(\frac{1}{r_2} - \frac{1}{r_1}\right)
    • D) W=−GMm(1r1+1r2)W = -GMm\left(\frac{1}{r_1} + \frac{1}{r_2}\right)
  4. 4.

    An object of mass mm is raised from the surface of a spherical planet of radius RR and mass MM to a height hh above the surface. Expressed in terms of the surface gravitational acceleration g=GMR2g = \frac{GM}{R^2}, what is the exact change in gravitational potential energy ΔU\Delta U of the object-planet system?

    • A) ΔU=mgh(1+hR)\Delta U = mgh\left(1 + \frac{h}{R}\right)
    • B) ΔU=mgh(1+hR)2\Delta U = \frac{mgh}{\left(1 + \frac{h}{R}\right)^2}
    • C) ΔU=mgh1+hR\Delta U = \frac{mgh}{1 + \frac{h}{R}}
    • D) ΔU=mgh1−hR\Delta U = \frac{mgh}{1 - \frac{h}{R}}
  5. 5.

    A satellite of mass mm moves in a circular orbit of radius rr around a planet of mass MM. Taking the gravitational potential energy of the system to be zero at infinite separation, what is the satellite's kinetic energy expressed in terms of the system's gravitational potential energy UU?

    • A) −12U-\frac{1}{2}U
    • B) −U-U
    • C) 12U\frac{1}{2}U
    • D) −2U-2U
  6. 6.

    Three identical particles, each of mass mm, are situated at the vertices of an equilateral triangle of side length LL. Taking the gravitational potential energy to be zero at infinite separation, what is the total gravitational potential energy of this three-particle system?

    • A) −3Gm2L-\frac{3Gm^2}{L}
    • B) −Gm2L-\frac{Gm^2}{L}
    • C) −3Gm22L-\frac{3Gm^2}{2L}
    • D) −Gm23L-\frac{Gm^2}{3L}
  7. 7.

    An object of mass mm is released from rest at a distance of 4R4R from the center of a spherical planet of mass MM and radius RR. Neglecting any atmospheric resistance, what is the speed of the object immediately before it reaches the surface of the planet?

    • A) 3GM4R\sqrt{\frac{3GM}{4R}}
    • B) 3GM2R\sqrt{\frac{3GM}{2R}}
    • C) GM2R\sqrt{\frac{GM}{2R}}
    • D) 2GMR\sqrt{\frac{2GM}{R}}
  8. 8.

    What is the minimum work that an external agent must perform to move a body of mass mm from the surface of a spherical planet of mass MM and radius RR to an infinite distance away, bringing it to rest?

    • A) GMmR\frac{GMm}{R}
    • B) -GMmR\frac{GMm}{R}
    • C) GMm2R\frac{GMm}{2R}
    • D) 2GMmR\frac{2GMm}{R}
  9. 9.

    Taking the gravitational potential energy of a two-body system to be zero at infinite separation, the gravitational potential energy at a finite separation rr is given by U(r)=−GMmrU(r) = -\frac{GMm}{r}. What does the negative sign of U(r)U(r) physically indicate about the system?

    • A) The gravitational force between the two masses is repulsive at all finite separations.
    • B) The total mechanical energy of the two-body system must always be strictly zero.
    • C) Energy is released by the system when the two masses are separated from distance rr to infinity.
    • D) The system is bound, meaning positive external work is required to separate the masses to infinity.
  10. 10.

    A spacecraft of mass mm is moved from an initial orbital radius of RR to a new orbital radius of 3R3R around a planet of mass MM. What is the change in gravitational potential energy, ΔU=Ufinal−Uinitial\Delta U = U_{\text{final}} - U_{\text{initial}}, of the planet-spacecraft system?

    • A) −2GMm3R-\frac{2GMm}{3R}
    • B) −GMm3R-\frac{GMm}{3R}
    • C) 2GMm3R\frac{2GMm}{3R}
    • D) 4GMm3R\frac{4GMm}{3R}

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