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Cavalieri's principle

Statement

If two solids in three-dimensional space lie between two parallel planes z=az = a and z=bz = b, and every plane z=tz = t (a≤t≤ba \le t \le b) parallel to those planes intersects the two solids in cross-sections of equal area A1(t)=A2(t)A_1(t) = A_2(t), then the two solids have equal volume: V1=V2V_1 = V_2.

Why is it true?

Imagine two identical stacks of thin coins of height b−ab - a. Even if you push one stack sideways into a tilted or curved shape, every horizontal slice at height tt still cuts through the exact same coin area A1(t)=A2(t)A_1(t) = A_2(t), and sliding the coins horizontally never creates or destroys volume — so the total volume V1=V2V_1 = V_2 is unchanged.

Proof sketch

By Fubini's theorem (or the cross-sectional volume formula in integral calculus), the volume of a solid bounded between z=az = a and z=bz = b with integrable cross-sectional area Ai(t)A_i(t) at height z=tz = t is the definite integral Vi=∫abAi(t) dtV_i = \int_a^b A_i(t)\,dt. Since A1(t)=A2(t)A_1(t) = A_2(t) for every t∈[a,b]t \in [a, b], their integrals over [a,b][a, b] are equal: V1=∫abA1(t) dt=∫abA2(t) dt=V2V_1 = \int_a^b A_1(t)\,dt = \int_a^b A_2(t)\,dt = V_2.

Topics that use this theorem

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Step-by-step proofs

No step-by-step proof yet for this theorem.

References

  1. Bonaventura Cavalieri (1635). Geometria indivisibilibus continuorum nova quadam ratione promota
  2. Carl B. Boyer, Uta C. Merzbach (2011). A History of Mathematics