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
Author: Deborah Hughes-Hallett, William G. McCallum, Andrew M. Gleason, Daniel E. Flath, Patti Frazer Lock, Sheldon P. Gordon, David O. Lomen, David Lovelock, Brad G. Osgood, Andrew Pasquale, Douglas Quinney, Jeff Tecosky-Feldman, Joseph Thrash, Karen R. Rhea, Thomas W. Tucker
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 .
4. Use method of separation of variable to solve the following wave equation
მłu
J²u
subject to
u(0,t) =0, for t> 0,
u(л,t) = 0, for t> 0,
=
t> 0,
at²
ax²'
u(x, 0) = 0,
0.01 x,
ut(x, 0) =
Π
0.01 (π-x),
0
Solve the following heat equation by method of separation variables:
ди
=
at
subject to
u(0,t) =0, for
-16024
ძx2 •
t>0, 0 0,
ux (4,t) = 0, for
t> 0,
u(x, 0) =
(x-3,
\-1,
0 < x ≤2
2≤ x ≤ 4.
ex
5.
important aspects.
Graph f(x)=lnx. Be sure to make your graph big enough to easily read (use the space given.) Label all
6
33
Chapter 4 Solutions
Calculus: Single And Multivariable, 7e Student Solutions Manual
Need a deep-dive on the concept behind this application? Look no further. Learn more about this topic, calculus and related others by exploring similar questions and additional content below.
01 - What Is A Differential Equation in Calculus? Learn to Solve Ordinary Differential Equations.; Author: Math and Science;https://www.youtube.com/watch?v=K80YEHQpx9g;License: Standard YouTube License, CC-BY
Higher Order Differential Equation with constant coefficient (GATE) (Part 1) l GATE 2018; Author: GATE Lectures by Dishank;https://www.youtube.com/watch?v=ODxP7BbqAjA;License: Standard YouTube License, CC-BY