Conservation of energy Suppose an object with mass m moves in a region R in a conservative force field given by F = -Vọ, where o is a potential function in a region R. The motion of the object is governed by Newton's Second Law of Motion, F = ma, where a is the acceleration. Suppose the object moves from point A to point B in R. dv a. Show that the equation of motion is m - -Vọ. dt 1 d 2 dt c. Take the dot product of both sides of the equation in part (a) with v(t) = r'(t) and integrate along a curve between A and B. Use part (b) and the fact that F is conservative to show that dv b. Show that - dt the total energy (kinetic plus potential) - m|v]² + q is the same at A and B. Conclude that because A and B are arbitrary, energy is conserved in R.

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Conservation of energy Suppose an object with mass m moves in
a region R in a conservative force field given by F = -Vọ, where
o is a potential function in a region R. The motion of the object is
governed by Newton's Second Law of Motion, F = ma, where
a is the acceleration. Suppose the object moves from point A to
point B in R.
dv
a. Show that the equation of motion is m -
-Vọ.
dt
1 d
2 dt
c. Take the dot product of both sides of the equation in part (a)
with v(t) = r'(t) and integrate along a curve between A and
B. Use part (b) and the fact that F is conservative to show that
dv
b. Show that -
dt
the total energy (kinetic plus potential) - m|v]² + q is the
same at A and B. Conclude that because A and B are arbitrary,
energy is conserved in R.
Transcribed Image Text:Conservation of energy Suppose an object with mass m moves in a region R in a conservative force field given by F = -Vọ, where o is a potential function in a region R. The motion of the object is governed by Newton's Second Law of Motion, F = ma, where a is the acceleration. Suppose the object moves from point A to point B in R. dv a. Show that the equation of motion is m - -Vọ. dt 1 d 2 dt c. Take the dot product of both sides of the equation in part (a) with v(t) = r'(t) and integrate along a curve between A and B. Use part (b) and the fact that F is conservative to show that dv b. Show that - dt the total energy (kinetic plus potential) - m|v]² + q is the same at A and B. Conclude that because A and B are arbitrary, energy is conserved in R.
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