Chapter XX: The Equality of Inertial and Gravitational Mass as an Argument for the General Postulate of Relativity

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12 Terms

1
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What is the ideal condition for applying Galilean mechanics in space?

A region far from stars or masses, where objects remain at rest or in uniform motion—defining a Galilean reference body.

2
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What scenario does Einstein use to model an accelerated reference frame?

A man inside a chest (room-like box) in space, pulled by a rope with constant force, causing uniform acceleration.

3
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How does the man inside the accelerating chest perceive his environment?

As if he is standing in a gravitational field—he feels a downward force and objects fall to the floor.

4
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What observation leads the man in the chest to conclude he's in a gravitational field?

All released objects accelerate downward at the same rate, regardless of their composition or mass.

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What discovery reinforces the man’s interpretation of a gravitational field?

He sees the rope and hook pulling the chest, suggesting it is suspended in a uniform gravitational field.

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Does Einstein believe the man’s interpretation is valid?

Yes—it does not violate reason or known mechanical laws, supporting an extension of relativity to accelerated frames.

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What principle allows the man to interpret acceleration as gravity?

The equality of inertial and gravitational mass, which ensures all bodies fall identically in a gravitational field.

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How do different observers explain the tension in a rope suspending a mass inside the chest?

  • Man in chest: Tension opposes gravitational pull on the body.

  • Free observer in space: Tension causes inertial acceleration of the body.

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What does this dual explanation of tension illustrate?

That gravitational mass = inertial mass, providing a physical interpretation for this law via the principle of equivalence.

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What key insight does the chest thought experiment provide for general relativity?

That accelerated reference frames can be interpreted as experiencing gravitational fields—leading to the general postulate of relativity.

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Can gravitational fields always be “transformed away” by switching reference frames?

No—only for special cases.

For example, the Earth’s gravitational field cannot be fully eliminated by changing reference frames.

12
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Why doesn’t the observer in the train (from Chapter XVIII) disprove the general principle of relativity?

Because he can interpret the braking force as a time-varying gravitational field, not necessarily a real acceleration.