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Solutions manual for mechanics and thermodynamics

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81

4.A particle that hangs from a spring oscillates with an angular frequency !. The spring-particle system is suspended from the ceiling of an elevator car and hangs motionless (relative to the elevator car), as the car descends at a constant speed v. The car then stops suddenly. Derive a formula for the amplitude with which the particle oscillates. (Assume the mass of the spring is negligible.) [Serway, 5th ed., pg. 415, Problem 14]

SOLUTION

The total energy is

E = K + U = 12mv2 + 12kx2

When v = 0, x = A giving

E = 12kA2

which is a constant and is the constant value of the total energy always. For the spring in the elevator we have the speed = v when x = 0. Thus

E =

 

1

kA2

=

 

1

mv2

+

 

1

kx2

2

2

2

 

 

 

 

 

 

 

 

 

 

=

1

mv2

+ O

 

 

 

 

2

 

 

 

 

 

 

 

 

 

 

Thus

A2 = mk v2

q

but ! = mk giving !2 = mk or mk = !12

A2 = v2 !2

v A = !

82

CHAPTER 12. OSCILLATIONS

5.A large block, with a second block sitting on top, is connected to a spring and executes horizontal simple harmonic motion as it slides across a frictionless surface with an angular frequency !. The coe±- cient of static friction between the two blocks is s. Derive a formula for the maximum amplitude of oscillation that the system can have if the upper block is not to slip. (Assume that the mass of the spring is negligible.) [Serway, 5th ed., pg. 418, Problem 54]

SOLUTION

Consider the upper block (of mass m),

F = ma

=sN

=smg

so that the maximum acceleration that the upper block can experience without slipping is

a = sg

the acceleration of the whole system is (with the mass of the lower block being M)

F= (M + m)a

=°kx

The maximum acceleration occurs when x is maximum, i.e. x = amplitude = A, giving the magnitude of a as

kA a = M + m

q

But ! = k giving a = A!2 = sg, i.e.

M+m

A = sg !2

83

6.A simple pendulum consists of a ball of mass M hanging from a uniform string of mass m, with m ø M (m is much smaller than M). If the period of oscillation for the pendulum is T , derive a formula for the speed of a transverse wave in the string when the pendulum hangs at rest. [Serway, 5th ed., pg. 513, Problem 16]

SOLUTION

The period of a pendulum is given by

s

T = 2º L g

where L is the length of the pendulum. The speed of a transverse wave on a string is rø

v =

where ø is the tension and is the mass per unit length. Newton's law gives (neglecting the mass of the string m)

F= Ma

ø° Mg = 0

ø = Mg

and the mass per unit length is

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

=

m

 

 

 

 

 

 

 

 

 

L

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

Thus

 

v = s

 

 

 

= s

 

 

 

 

 

 

 

 

 

 

 

m

 

 

 

m=L

 

 

 

 

 

 

 

Mg

 

 

 

 

 

MgL

 

T 2g

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

but T 2 = 4º2 L or L =

giving

 

 

 

 

 

 

 

 

 

2

 

 

 

 

 

 

 

 

 

g

4º

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

v = s

 

 

 

 

 

2º s

 

 

 

 

m4º2

=

 

 

m

 

 

 

 

 

MgT 2g

gT M

84

CHAPTER 12. OSCILLATIONS

Chapter 13

WAVES - I

85

86

CHAPTER 13. WAVES - I

Chapter 14

WAVES - II

87

88

CHAPTER 14. WAVES - II

1.A uniform rope of mass m and length L is suspended vertically. Derive a formula for the time it takes a transverse wave pulse to travel the length of the rope.

(Hint: First Ønd an expression for the wave speed at any point a distance x from the lower end by considering the tension in the rope as resulting from the weight of the segment below that point.) [Serway, 5th ed., p. 517, Problem 59]

SOLUTION

Consider a point a distance x from the lower end, assuming the rope

has a uniform linear mass density = mL . The mass below the point is

m = x

and the weight of that mass will produce tension T in the rope above

T = mg = xg

(This agrees with our expectation. The tension at the bottom of the rope (x = 0) is T = 0, and at the top of the rope (x = L) the tension is T = Lg = mg.)

The wave speed is

v = s

 

 

= r

 

= pxg

 

 

 

 

 

T

xg

 

 

The speed is deØned as v ¥ dxdt and the time is dt = dxv . Integrate this to get the total time to travel the length of the rope

t =

Z0

dt = Z0

v

= pg Z0

px

 

t

 

 

 

L dx

1

 

L dx

= pg h2x1=2i0

 

 

 

 

 

 

 

 

 

 

 

1

 

 

 

L

 

 

 

 

 

 

 

 

2p

 

 

 

 

 

 

 

 

=

1

 

 

 

 

 

 

 

 

L

 

 

 

 

 

 

 

p

 

 

 

 

 

 

 

 

 

 

 

g

 

 

 

 

 

 

s

=2 L g

89

2.A uniform cord has a mass m and a length L. The cord passes over a pulley and supports an object of mass M as shown in the Øgure. Derive a formula for the speed of a wave pulse travelling along the cord. [Serway, 5 ed., p. 501]

L - x

x

M

SOLUTION

The tension T in the cord is equal to the weight of the mass M or

X

F = Ma

T° Mg = 0

T = Mg

q

The wave speed is v = T where is the mass per unit length

 

 

 

=

m

 

 

 

 

L

 

 

 

 

 

Thus

s

 

 

 

 

s

 

 

 

 

 

v =

Mg

 

=

MgL

 

 

 

 

m=L

 

m

 

 

 

90

CHAPTER 14. WAVES - II

3.A block of mass M, supported by a string, rests on an incline making an angle µ with the horizontal. The string's length is L and its mass is m ø M (i.e. m is negligible compared to M). Derive a formula for the time it takes a transverse wave to travel from one end of the string to the other. [Serway, 5th ed., p. 516, Problem 53]

L

M

θ

SOLUTION

 

 

 

The wave speed is given by v =

 

where T is the tension in the

T

 

 

 

 

length = m

. To get the tension,

string and is the mass per unit q

 

L

use Newton's laws as shown in the Øgure below.