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Gravitation - Gravitational Potential Energy

Grade 11CBSEPhysics

Review the key concepts, formulae, and examples before starting your quiz.

πŸ”‘Concepts

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The gravitational potential energy (UU) of a body at a point is defined as the work done by an external agent in bringing the body from infinity to that point without acceleration.

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Gravitational potential energy is a scalar quantity. Its SI unit is Joule (JJ) and its dimensional formula is [M1L2Tβˆ’2][M^1 L^2 T^{-2}].

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The reference point for zero gravitational potential energy is typically taken at infinity (r=∞r = \infty).

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The negative sign in the expression U=βˆ’GMmrU = -\frac{GMm}{r} signifies the attractive nature of the gravitational force, indicating that the system is bound.

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Gravitational potential (VV) is defined as the gravitational potential energy per unit mass: V=UmV = \frac{U}{m}.

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For a body near the surface of the Earth (hβ‰ͺReh \ll R_e), the change in potential energy can be approximated as Ξ”U=mgh\Delta U = mgh, where g=GMeRe2g = \frac{GM_e}{R_e^2}.

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The work done in moving a mass mm from distance r1r_1 to r2r_2 is given by W=U(r2)βˆ’U(r1)=GMm(1r1βˆ’1r2)W = U(r_2) - U(r_1) = G M m \left( \frac{1}{r_1} - \frac{1}{r_2} \right).

πŸ“Formulae

U=βˆ’GMmrU = -\frac{G M m}{r}

V=βˆ’GMrV = -\frac{G M}{r}

Ξ”U=GMm(1Reβˆ’1Re+h)\Delta U = G M m \left( \frac{1}{R_e} - \frac{1}{R_e + h} \right)

Ξ”U=mgh1+hRe\Delta U = \frac{mgh}{1 + \frac{h}{R_e}}

Usurface=βˆ’GMemReU_{surface} = -\frac{G M_e m}{R_e}

πŸ’‘Examples

Problem 1:

Calculate the change in gravitational potential energy when a body of mass mm is raised from the surface of the Earth to a height hh equal to the radius of the Earth ReR_e.

Solution:

The initial potential energy at the surface is Ui=βˆ’GMemReU_i = -\frac{GM_em}{R_e}. The final potential energy at height h=Reh = R_e (total distance r=2Rer = 2R_e) is Uf=βˆ’GMem2ReU_f = -\frac{GM_em}{2R_e}. The change in potential energy is Ξ”U=Ufβˆ’Ui=βˆ’GMem2Reβˆ’(βˆ’GMemRe)=GMem2Re\Delta U = U_f - U_i = -\frac{GM_em}{2R_e} - (-\frac{GM_em}{R_e}) = \frac{GM_em}{2R_e}. Since g=GMeRe2g = \frac{GM_e}{R_e^2}, we can substitute GMe=gRe2GM_e = gR_e^2, giving Ξ”U=m(gRe2)2Re=12mgRe\Delta U = \frac{m(gR_e^2)}{2R_e} = \frac{1}{2}mgR_e.

Explanation:

This demonstrates that for large heights, the simple mghmgh formula is inaccurate. Using mghmgh would yield mgRemgR_e, which is double the actual value required to reach that altitude.

Problem 2:

Find the gravitational potential at a point on the surface of the Earth. (Given: Me=6Γ—1024Β kgM_e = 6 \times 10^{24} \text{ kg}, Re=6.4Γ—106Β mR_e = 6.4 \times 10^6 \text{ m}, G=6.67Γ—10βˆ’11Β NΒ m2kgβˆ’2G = 6.67 \times 10^{-11} \text{ N m}^2\text{kg}^{-2})

Solution:

Using the formula for gravitational potential V=βˆ’GMeReV = -\frac{GM_e}{R_e}: V=βˆ’6.67Γ—10βˆ’11Γ—6Γ—10246.4Γ—106V = -\frac{6.67 \times 10^{-11} \times 6 \times 10^{24}}{6.4 \times 10^6} Vβ‰ˆβˆ’6.25Γ—107Β J/kgV \approx -6.25 \times 10^7 \text{ J/kg}

Explanation:

Gravitational potential represents the work done per unit mass. The negative value indicates that work must be done against the gravitational field to move the mass to infinity.

Gravitational Potential Energy - Revision Notes & Key Formulas | CBSE Class 11 Physics