Problems 57–58 use the fact that a physical system is in stable equilibrium if the total energy, E , is a local minimum . 7 A mass m hanging on the end of a spring extends its length by y . See Figure 4.55. For g , the acceleration due to gravity, and positive constant k , the total energy is E = 1 2 k y 2 − m g y . Is there a length that gives a stable equilibrium position for a constant mass m ? If so, what is it? Figure 4.55
Problems 57–58 use the fact that a physical system is in stable equilibrium if the total energy, E , is a local minimum . 7 A mass m hanging on the end of a spring extends its length by y . See Figure 4.55. For g , the acceleration due to gravity, and positive constant k , the total energy is E = 1 2 k y 2 − m g y . Is there a length that gives a stable equilibrium position for a constant mass m ? If so, what is it? Figure 4.55
Problems 57–58 use the fact that a physical system is in stable equilibrium if the total energy, E, is a local minimum.7
A mass m hanging on the end of a spring extends its length by y. See Figure 4.55. For g, the acceleration due to gravity, and positive constant k, the total energy is
E
=
1
2
k
y
2
−
m
g
y
.
Is there a length that gives a stable equilibrium position for a constant mass m? If so, what is it?
Figure 4.55
Formula Formula A function f(x) attains a local maximum at x=a , if there exists a neighborhood (a−δ,a+δ) of a such that, f(x)<f(a), ∀ x∈(a−δ,a+δ),x≠a f(x)−f(a)<0, ∀ x∈(a−δ,a+δ),x≠a In such case, f(a) attains a local maximum value f(x) at x=a .
For each given function f(x) find f'(x) using the rules learned in section 9.5.
1. f(x)=x32
32x
2. f(x)=7x+13
3. f(x) =
x4
4. f(x) = √√x³
5. f(x) = 3x²+
3
x2
Find:
lim x →-6 f (x)
limx-4 f (x)
lim x-1 f (x)
lim x →4 f (x)
(-6,3) •
(-1,5)
-8
-7
(-6,-2)
4+
(4,5)
(4,2) •
(-1,1)
-6
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