A mass m is accelerated by a time-varying force e-ßt v3, where v is its velocity. It also experiences a resistive force nv, where n is a constant, owing to its motion through the air. The equation of motion of the mass is therefore dv m- = e dt Solve this to show that 1 1 2 2n v2 ßt + e mß + n m mß + n.
A mass m is accelerated by a time-varying force e-ßt v3, where v is its velocity. It also experiences a resistive force nv, where n is a constant, owing to its motion through the air. The equation of motion of the mass is therefore dv m- = e dt Solve this to show that 1 1 2 2n v2 ßt + e mß + n m mß + n.
Algebra & Trigonometry with Analytic Geometry
13th Edition
ISBN:9781133382119
Author:Swokowski
Publisher:Swokowski
Chapter2: Equations And Inequalities
Section2.7: More On Inequalities
Problem 44E
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