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Gravitation - Gravitational Potential Energy

Grade 11CBSEPhysics

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

šŸ”‘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 [M1L2Tāˆ’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=āˆžr = \infty).

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The negative sign in the expression U=āˆ’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 (h≪Reh \ll R_e), the change in potential energy can be approximated as Ī”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)āˆ’U(r1)=GMm(1r1āˆ’1r2)W = U(r_2) - U(r_1) = G M m \left( \frac{1}{r_1} - \frac{1}{r_2} \right).

šŸ“Formulae

U=āˆ’GMmrU = -\frac{G M m}{r}

V=āˆ’GMrV = -\frac{G M}{r}

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

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

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

šŸ’”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=āˆ’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=āˆ’GMem2ReU_f = -\frac{GM_em}{2R_e}. The change in potential energy is Ī”U=Ufāˆ’Ui=āˆ’GMem2Reāˆ’(āˆ’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 Ī”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=6Ɨ1024Ā kgM_e = 6 \times 10^{24} \text{ kg}, Re=6.4Ɨ106Ā mR_e = 6.4 \times 10^6 \text{ m}, G=6.67Ɨ10āˆ’11Ā NĀ m2kgāˆ’2G = 6.67 \times 10^{-11} \text{ N m}^2\text{kg}^{-2})

Solution:

Using the formula for gravitational potential V=āˆ’GMeReV = -\frac{GM_e}{R_e}: V=āˆ’6.67Ɨ10āˆ’11Ɨ6Ɨ10246.4Ɨ106V = -\frac{6.67 \times 10^{-11} \times 6 \times 10^{24}}{6.4 \times 10^6} Vā‰ˆāˆ’6.25Ɨ107Ā 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.