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Solutions manual for mechanics and thermodynamics

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Chapter 6

KINETIC ENERGY & WORK

51

52

CHAPTER 6. KINETIC ENERGY & WORK

Chapter 7

POTENTIAL ENERGY & CONSERVATION OF ENERGY

53

54CHAPTER 7. POTENTIAL ENERGY & CONSERVATION OF ENERGY

1.A block of mass m slides down a rough incline of height H and angle µ to the horizontal. Calculate the speed of the block when it reaches the bottom of the incline, assuming the coe±cient of kinetic friction

is k.

SOLUTION

The situation is shown in the Øgure.

y

Fk

N

 

H

 

θ

W

cos

 

W

sin

 

 

θ

θ 90

 

x

θ

 

θ x

W

55

The work-energy theorem is

¢U + ¢K = WNC

= Uf ° Ui + Kf ° Ki

but Uf = 0 and Ki = 0 giving

KF = Ui + WNC

Obviously WNC must be negative so that Kf < Ui

 

KF

=

Ui ° Fk¢x

where

¢x =

H

 

 

1

sin µ

mv2

=

mgH ° kN

H

 

 

 

 

 

 

 

2

sin µ

 

 

where we have used Fk = kN. To get N use Newton's law

F

=

ma

N ° W cos µ

=

0

N

=

W cos µ

 

=

mg cos µ

)

1

mv2

=

mgH ° kmg cos µ

H

2

sin µ

 

 

v2

=

2gH ° 2 kg

H

 

 

 

 

 

 

 

 

 

tan µ

 

 

 

=

2gH(1 °

k

 

 

 

 

 

)

 

 

 

 

 

tan µ

 

 

v

=

r

 

 

 

 

 

 

2gH(1 ° tan µ )

 

 

 

 

 

 

 

k

 

 

56CHAPTER 7. POTENTIAL ENERGY & CONSERVATION OF ENERGY

Chapter 8

SYSTEMS OF PARTICLES

57

58

CHAPTER 8. SYSTEMS OF PARTICLES

1.A particle of mass m is located on the x axis at the position x = 1 and a particle of mass 2m is located on the y axis at position y = 1 and

a third particle of mass m is located oÆ-axis at the position (x; y) = (1; 1). What is the location of the center of mass?

SOLUTION

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

The position of the center of mass is

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

1

Xi

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

~rcm =

 

mi~ri

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

M

 

 

 

 

 

 

 

 

 

with M ¥ Pi

mi. The x and y coordinates are

 

 

 

 

 

xcm = M Xi

mixi

 

 

 

and ycm = M Xi

miyi

 

 

 

 

1

 

 

 

 

 

 

 

 

 

 

 

1

 

 

 

 

 

 

=

 

 

 

 

1

£

 

 

 

 

 

=

 

 

 

1

£

 

 

 

 

 

 

 

 

 

 

 

 

 

 

m + 2m + m

 

 

 

 

 

m + 2m + m

 

 

£(m £ 1 + 2m £ 0 + m £ 1)

£(m £ 0 + 2m £ 1 + m £ 1)

=

1

(m + 0 + m) =

2m

=

1

 

(0 + 2m + m) =

3m

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

4m

4m

4m

 

4m

 

 

 

 

 

 

 

=

1

 

 

 

 

 

 

 

 

 

 

 

=

3

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

2

 

 

 

 

 

 

 

 

 

 

 

4

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

Thus the coordinates of the center of mass are

µ1 3 (xcm; ycm) = 2; 4

59

2.Consider a square at table-top. Prove that the center of mass lies at the center of the table-top, assuming a constant mass density.

SOLUTION

Let the length of the table be L and locate it on the x{y axis so that one corner is at the origin and the x and y axes lie along the sides of the table. Assuming the table has a constant area mass density æ, locate the position of the center of mass.

xcm = M

i

mixi = M Z

x dm

 

 

1

X

1

 

 

 

 

 

=

M

Z

 

x ædA

with æ = dA =

A

 

1

 

 

 

 

 

dm

M

 

 

 

Z

 

 

 

 

 

 

 

 

=

æ

 

x dA

if æ is constant

 

 

 

 

 

M

 

 

=

1

 

Z L Z L x dx dy

with A = L2

 

 

00

=1 1x2 L [y]L

A 2 0 0A

=

1 1

L2 £ L =

L3

L3

 

 

 

 

=

 

A

2

2A

2L2

=12L

and similarly for

 

Z

y dA = 2L

ycm = M

æ

 

1

Thus

1

 

1

 

(xcm; ycm) = µ

L;

L as expected

 

 

 

2

2

60

CHAPTER 8. SYSTEMS OF PARTICLES

3.A child of mass mc is riding a sled of mass ms moving freely along an icy frictionless surface at speed v0. If the child falls oÆ the sled, derive a formula for the change in speed of the sled. (Note: energy is not conserved !) WRONG WRONG WRONG ??????????????

speed of sled remains same - person keeps moving when fall oÆ ???????

SOLUTION

Conservation of momentum in the x direction is

XX

pix = pfx

(mc + ms)v0 = msv where v is the new Ønal speed of the sled, or

v =

µ1 + ms v0

 

 

mc

the change in speed is

v ° v0 = mc v0 ms

which will be large for small ms or large mc.