Copyright © 2012 Pearson Education Inc. Stress, Strain, and elastic moduli Physics 7C lecture 16...

Copyright © 2012 Pearson Education Inc.

Stress, Strain, and elastic moduli

Physics 7C lecture 16

Tuesday November 26, 8:00 AM – 9:20 AMEngineering Hall 1200


Strain, stress, and elastic moduli

• Stretching, squeezing, and twisting a real body causes it to deform, as shown in figure below. We shall study the relationship between forces and the deformations they cause.

• Stress is the force per unit area and strain is the fractional deformation due to the stress. Elastic modulus is stress divided by strain.

• The proportionality of stress and strain is called Hooke’s law.


Strain, stress, and elastic moduli

StressElastic modulus

Strain=

force per unit dimension

fractional deformation

molecular basis for Hook’s law:


Tensile and compressive stress and strain

• Tensile stress = F /A and tensile strain = l/l0. Compressive stress

and compressive strain are defined in a similar way.

• Young’s modulus is tensile stress divided by tensile strain, and is

given by Y = (F/A)(l0/l).



Young’s modulus = tensile stress / tensile strain,

Y = (F/A)(l0/l).

This is pressure! tiny!

setup for measuring Young’s modulus


Some values of elastic moduli



setup for measuring Young’s modulus

1 meter long steel string with 1 mm diameter, pulled by 10 N weight!

Ysteel = 20 X 1010 P

the elongation is

dL = L * F / (A Y)

= only 0.5 mm!


Tensile stress and strain

• In many cases, a body can experience both tensile and compressive stress at the same time.


A. more stress and more strain.

B. the same stress and more strain.

C. the same stress and less strain.

D. less stress and less strain.

E. the same stress and the same strain.

Q11.5

Two rods are made of the same kind of steel and have the same diameter.

FF length 2L

FF length L

A force of magnitude F is applied to the end of each rod. Compared to the rod of length L, the rod of length 2L has







A11.5

Two rods are made of the same kind of steel and have the same diameter.

FF length 2L

FF length L








Q11.6

Two rods are made of the same kind of steel. The longer rod has a greater diameter.

FF length 2L

FF length L








A11.6

Two rods are made of the same kind of steel. The longer rod has a greater diameter.

FF length 2L

FF length L



Bulk stress and strain


Bulk stress and strain

• Pressure in a fluid is force per unit area: p = F/A.

• Bulk stress is pressure change p and bulk strain is

fractional volume change

V/V0.

• Bulk modulus is bulk stress divided by bulk strain and is given by B = –p/(V/V0).


Anglerfish

1000 m deep sea

© 2012 Pearson Education, Inc.

Table 11.2

1/ bulk modulus = compressibilityk = 1/B

In 1000 meter deep sea, how much is water compressed?

dV/V = k * p

= 46.4E-6 atm-1* 100 atm

= 0.464 % !

water is very hard to compress!


Sheer stress and strain


Sheer stress and strain

• Sheer stress is F||/A and sheer strain is x/h, as shown in figure.

• Sheer modulus is sheer stress divided by sheer strain, and is given by S = (F||/A)(h/x).


Sheer stress and strain of brass

The left piece experience shear force in an earthquake. It is 0.8 m square and 0.5 cm thick. What is the force exerted on each of its edges if the displacement is x = 0.16 mm?

sol:

shear strain= x/h = 0.16 mm / 0.8 m = 0.0002

shear stress = shear strain * S = 0.0002 * 3.5E10 Pa = 7E6 Pa

force F = shear stress * A = 7E6 Pa * 0.8 m* 0.5 cm = 2.8E4 N

This is a huge force, even the displacement (0.16) is tiny!


Elasticity and plasticity

• Hooke’s law applies up to point a in Figure 11.18 below.

• Table 11.3 shows some approximate breaking stresses.


Midterm problem

A solid, uniform cylinder (radius r; mass m; moment of inertia around central axis I = ½ m r2) rolls without slipping up a hill, as shown in the figure. The initial speed is v0 and the height of the hill is h. At the top of the hill, it is moving horizontally, and then it goes over the vertical cliff.

(a) How far from the foot of the cliff does the cylinder land? (20 points)

(b) Calculate the linear speed v2 and angular speed ω2 when the cylinder lands. Is the total kinetic energy at that moment equal or smaller than the initial kinetic energy when the cylinder was at the initial speed v0? (20 points)


Midterm problem

Copyright © 2012 Pearson Education Inc. Stress, Strain, and elastic moduli Physics 7C lecture 16...

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