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2. Newtonian Mechanics Newton’s law Motion under constant forces

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Presentation on theme: "2. Newtonian Mechanics Newton’s law Motion under constant forces"— Presentation transcript:

1 2. Newtonian Mechanics Newton’s law Motion under constant forces
Position dependent forces Velocity dependent forces SOONGSIL UNIVERSITY CLASSICAL MECHANICS

2 2.2 Motion under a constant force
SOONGSIL UNIVERSITY CLASSICAL MECHANICS

3 Bottom 에서의 속도는? 마찰이 있을 때와 없을 때 마찰이 있을 때 마찰이 없을 때 SOONGSIL UNIVERSITY CLASSICAL MECHANICS

4 2.3 Position dependent force
Potential E can be defined as SOONGSIL UNIVERSITY CLASSICAL MECHANICS

5 v0 Free fall Maximum height of a ball thrown upward
2.3 Position dependent force continued Free fall v0 h Maximum height of a ball thrown upward For a given initial velocity, there always exists maximum height. Is it correct? SOONGSIL UNIVERSITY CLASSICAL MECHANICS

6 Variation of Gravity with height
2.3 Position dependent force continued Variation of Gravity with height Definition of the gravitational acceleration Escape speed SOONGSIL UNIVERSITY CLASSICAL MECHANICS

7 = + Morse function V(x) : potential energy of a diatomic molecule x
2.3 Position dependent force continued Morse function V(x) : potential energy of a diatomic molecule = + x Therefore, x=x0 is the equilibrium position. separation of the atoms and –V0 is the binding energy. SOONGSIL UNIVERSITY CLASSICAL MECHANICS

8 Near the equilibrium position V(x) can be expanded
2.3 Position dependent force continued Near the equilibrium position V(x) can be expanded The potential becomes parabolic in the leading order, And it can be considered as a simple harmonic oscillator problem. SOONGSIL UNIVERSITY CLASSICAL MECHANICS

9 Maximum separation at room temp.?
2.3 Position dependent force continued Hydrogen molecule Maximum separation at room temp.? Binding energy = eV Equilibrium separation = nm Delta = nm Room temp. ~ 1/40 eV X = nm ~3.6% change in size which means thermal expansion SOONGSIL UNIVERSITY CLASSICAL MECHANICS

10 2.4 velocity dependent force
in SI unit, The ratio SOONGSIL UNIVERSITY CLASSICAL MECHANICS

11 As time goes to infinity, it converges to a point.
2.3 velocity dependent force continued linear resistance (Dominant in low speed) quadratic resistance (Dominant in high speed) As time goes to infinity, it converges to a point. As time goes to infinity, does it converge??? It shows logarithmic divergence!!! SOONGSIL UNIVERSITY CLASSICAL MECHANICS

12 vertical fall through a fluid (linear resistance)
mg -C1v As time goes to infinity, the velocity approaches to –mg/c1. Terminal velocity where the terminal speed = , and = It occurs when F = 0. If an object is dropped, after , v = vt SOONGSIL UNIVERSITY CLASSICAL MECHANICS

13 vertical fall through a fluid (quadratic resistance)
If an object is dropped, after , v = vt SOONGSIL UNIVERSITY CLASSICAL MECHANICS

14 Terminal speed of raindrops and basketballs
Raindrop ~ 0.1 mm Basketball ~ 0.25 m The ratio raindrops basketballs The ratio = 0.14 v v = 7.1m/s linear term dominates. The ratio = 350 v v = m/s quadratic term dominates. SOONGSIL UNIVERSITY CLASSICAL MECHANICS

15 The end 2. Newtonian Mechanics Newton’s law
Motion under constant forces Position dependent forces Velocity dependent forces The end SOONGSIL UNIVERSITY CLASSICAL MECHANICS


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