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How does the gravitational force between two masses depend on their masses and separation?

State Newton's law of universal gravitation, apply Fg=Gm1m2/r2F_g = Gm_1m_2/r^2 to calculate the gravitational force, and use the inverse-square relationship to reason about how the force changes with distance.

A Regents Physics answer on universal gravitation: Newton's law of gravitation, the inverse-square dependence on distance, the meaning of the gravitational field strength, and how to apply the Reference-Table equation, with worked examples and proportional reasoning.

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  1. What this topic is asking
  2. Newton's law of universal gravitation
  3. The inverse-square law
  4. Gravitational field strength and weight
  5. Reference Tables note
  6. Try this

What this topic is asking

Universal gravitation is Newton's account of the attractive force between any two masses, from a falling apple to the orbit of a planet. The Physical Setting/Physics course asks you to state the law, calculate the force with Fg=Gm1m2r2F_g = \dfrac{Gm_1 m_2}{r^2}, and reason with the inverse-square relationship: how the force changes when the masses or the distance change. The Regents tests both direct calculation and the proportional reasoning the inverse-square law invites.

Newton's law of universal gravitation

The force acts on both masses equally and oppositely (Newton's third law), no matter how different their sizes: Earth pulls a satellite with the same force the satellite pulls Earth. Gravity is always attractive, never repulsive, and it acts at a distance, with no contact needed. Because GG is tiny, the force is negligible between everyday objects and significant only when at least one mass is astronomical.

The inverse-square law

The inverse-square reasoning is a favorite Regents item, often without numbers. The procedure is to square the distance factor and invert it. The masses, by contrast, enter linearly: doubling one mass doubles the force, and doubling both quadruples it. Keeping the mass dependence (linear) separate from the distance dependence (inverse-square) avoids confusion.

Gravitational field strength and weight

Near a planet of mass MM and radius rr, the gravitational force on a small mass mm is its weight, and equating Fg=mgF_g = mg with the gravitation law gives the gravitational field strength:

g=GMr2g = \frac{GM}{r^2}

This explains why gg differs between planets (the Moon's smaller mass gives a smaller gg, about 1.61.6 m/s squared) and why gg decreases with altitude (larger rr). It also shows that the weight Fg=mgF_g = mg near a surface is just the universal law evaluated at that surface. The gravitational field is the region around a mass where another mass feels a force, and gg measures its strength in newtons per kilogram (equivalently m/s squared).

Reference Tables note

The Reference Tables print Fg=Gm1m2r2F_g = \dfrac{Gm_1 m_2}{r^2} and Fg=mgF_g = mg in the Mechanics section, and the constant G=6.67Γ—10βˆ’11G = 6.67 \times 10^{-11} N m squared per kg squared in the constants list, along with the masses and radii of Earth and other bodies on some editions. The field-strength form g=GMr2g = \dfrac{GM}{r^2} is not printed separately but follows by equating the two printed expressions. Gravity supplies the centripetal force for orbits, linking this topic to uniform circular motion.

Try this

Q1. State how the gravitational force between two masses changes if the distance between them is tripled. [1 point]

  • Cue. It becomes one ninth as large (inverse-square: 32=93^2 = 9).

Q2. State two factors that determine the gravitational force between two objects. [2 points]

  • Cue. The product of their masses, and the (inverse square of the) distance between their centers.

Exam-style practice questions

Practice questions written in the style of NYSED exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.

Regents (style)2 marksPart B-2 (constructed response). Two 5.05.0 kg masses are placed with their centers 2.02.0 m apart. Using G=6.67Γ—10βˆ’11G = 6.67 \times 10^{-11} N m squared per kg squared, calculate the gravitational force between them. Show the equation, substitution and answer.
Show worked answer β†’

A 2-point constructed-response calculation using the Reference-Table equation Fg=Gm1m2r2F_g = \dfrac{Gm_1 m_2}{r^2}.

Equation: Fg=Gm1m2r2F_g = \dfrac{Gm_1 m_2}{r^2}.
Substitution: Fg=(6.67Γ—10βˆ’11)(5.0)(5.0)(2.0)2=(6.67Γ—10βˆ’11)(25)4.0F_g = \dfrac{(6.67 \times 10^{-11})(5.0)(5.0)}{(2.0)^2} = \dfrac{(6.67 \times 10^{-11})(25)}{4.0}.
Answer: Fg=4.2Γ—10βˆ’10F_g = 4.2 \times 10^{-10} N (a very small attractive force).

Markers reward the equation from the tables, correct substitution including the constant GG and the squared distance, and an answer in newtons. A common error is forgetting to square the separation.

Regents (style)1 marksPart A (multiple choice). If the distance between two masses is doubled, the gravitational force between them becomes (1) twice as large (2) half as large (3) one quarter as large (4) four times as large. Justify your reasoning.
Show worked answer β†’

A 1-point Part A item on the inverse-square law. The answer is (3).

Gravitation follows an inverse-square law, Fg=Gm1m2r2F_g = \dfrac{Gm_1 m_2}{r^2}. Doubling the distance multiplies r2r^2 by four, so the force drops to one quarter of its original value. The trap is treating the relationship as simple inverse (half) instead of inverse-square (one quarter).

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