Young's Modulus and Material Strength Calculations

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44. (a) The Young’s modulus is given by

F1oWgVa2YMNde+8AZHtmKNqk0LPQGy9gj5C5Hrin

(b) Since the linear range of the curve extends to about 2.9 × 108 N/m2, this is approximately the yield strength for the material.

46. Since the force is (stress × area) and the displacement is (strain × length), we can write the work integral (eq. 7-32) as

  W = gif;base64,R0lGODlhKAAdAHcAMSH+GlNvZnR3Y

  = u2CgThlq1LxpdyJLjkcyUkMZOGNYqiRJJnpZrdsBA (differential strain)L  = AL u2CgThlq1LxpdyJLjkcyUkMZOGNYqiRJJnpZrdsB(differential strain)

which means the work is  (wire-area) × (wire-length) × (graph-area-under-curve).  Since the area of a triangle (see the graph in the problem statement) is  (base)(height)  then we determine the work done to be

            W = (2.00 x 10-6 m2)(0.800 m)(1.0 × 10-3)(7.0 × 107 N/m2) = 0.0560 J .

48. 46. Since the force is (stress × area) and the displacement is (strain × length), we can write the work integral (eq. 7-32) as

  W = gif;base64,R0lGODlhKAAdAHcAMSH+GlNvZnR3Y

  = u2CgThlq1LxpdyJLjkcyUkMZOGNYqiRJJnpZrdsBA (differential strain)L  = AL u2CgThlq1LxpdyJLjkcyUkMZOGNYqiRJJnpZrdsB(differential strain)

which means the work is  (thread cross-sectional area) × (thread length) × (graph-area-under-curve). The area under the curve is 

u3pAkQb5YJyRmb3PkZVauZt+mZugm4jouSFSaNLQ

(a) The kinetic energy that would put the thread on the verge of breaking is simply equal to W:

            a+A2YsMGojLIA7ULYDNKgn1DlheDJbmDoOfGWEHT

(b) The kinetic energy of the fruit fly of mass 6.00 mg and speed 1.70 m/s is

                                           RJqBHy4GGfmFYTBWaAn44nUFfKBPf4Z4ib6iQK5B

(c) Since gif;base64,R0lGODlhNwAZAHcAMSH+GlNvZnR3Y

, the fruit fly will not be able to break the thread.

(d) The kinetic energy of a bumble bee of mass 0.388 g and speed 0.420 m/s is

gJDlnCjWyMoxwtEbhH1EdxjnjM4yB8Bwk+6vGPgK

(e) On the other hand, since gif;base64,R0lGODlhNQAYAHcAMSH+GlNvZnR3Y

, the bumble bee will be able to break the thread.

49. The flat roof (as seen from the air) has area A = 150 m × 5.8 m = 870 m2. The volume of material directly above the tunnel (which is at depth d = 60 m) is therefore

V = A × d = (870 m2) × (60m) = 52200 m3.

Since the density is r = 2.8 g/cm3 = 2800 kg/m3, we find the mass of material supported by the steel columns to be m = rV = 1.46 × 108 m3.

(a) The weight of the material supported by the columns is mg = 1.4 × 109 N.

(b) The number of columns needed is

fqNlG2hSKAGJIev8DoPNyAyibFCsdlrtio44Txtu

50. On the verge of breaking, the length of the thread is

..\figures\jpg\12-50.jpg

VYfhfhZuP+YUDjJAtEEEq414GdRdJAIhAjOptUkL

,

where  dYJ8gw8SkF4TFIiWiEKZm5dLFYucAKKUo56lTWxW

is the original length, and QIBwSCwahQbB4MhsGg0EYyFAPSCMCUVxWr06v0gB

, as given in the problem. The free-body diagram of the system is shown on the right. The condition for equilibrium is

0wKqk3DUGqVfS4FauDwZmRKM2qXUg1SMgkMKYI8M

where m is the mass of the insect and  WAQXfgBydIdYEBhzQ3tWBhmGj1YLSUsLbZpWBBps

. Since the volume of the thread remains constant is it is being stretched, we have CAVoskTjMoASLJtgQvBjRhEOrkZTshztUrRpvJww

, or 3qi6V7jMvQeXBFIOefHRzxcLAgA7

. The vertical distance gif;base64,R0lGODlhFwAVAHcAMSH+GlNvZnR3Y

 is

YH7Eb++wvgHvonwAKOj4ABDAIAOw==

.

Thus, the mass of the insect is

AJEIopo1qWIYd4TU4FeiroBYwIViq5HSPiWEC6me

or 0.421 g.

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