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complete Solutions Manual for Metal Forming: Mechanics and Metallurgy, 4th Edition by Hosford & Caddell.(PDF)

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INSTANT PDF DOWNLOAD – Access the complete Solutions Manual for Metal Forming: Mechanics and Metallurgy, 4th Edition by Hosford & Caddell. Includes step-by-step solutions, detailed explanations, and problem-solving techniques for all chapters. Perfect for materials and mechanical engineering students preparing for assignments and exams. High-quality PDF for instant access and efficient studying. metal forming, solutions manual, metallurgy pdf, engineering exam, study guide, homework help, pdf download, materials engineering metal forming solutions manual pdf, hosford caddell solutions manual download, metallurgy 4th edition solutions pdf, metal forming solved problems pdf, engineering metallurgy solutions manual, metal forming exam prep pdf, metal forming homework solutions pdf, metallurgy assignment answers pdf, metal forming study guide pdf download, metal forming solutions instant download, metallurgy problem solutions pdf, materials engineering solutions manual pdf, metal forming revision guide pdf, hosford metal forming answers pdf, metal forming all chapters solutions pdf, metallurgy exam questions and answers pdf, metal forming problem solving pdf download, metal forming solutions manual download, metallurgy solutions pdf, metal forming mechanics solutions pdf

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SOLUTION MANUAL

, Solution Manual 3rd Ed. Metal Forming: Mechanics and Metallurgỵ
Chapter 1


Determine the principal stresses for the stress state
10 −3 4
 ij = −3 5 2 .
4 2 7
Solution: I1 = 10+5+7=32, I2 = -(50+35+70) +9 +4 +16 = -126, I3 = 350 -48 -40 -80
-63 = 119;  – 222 -126 -119 = 0. A trial and error solution gives  -= 13.04.
3

฀ Factoring out 13.04, 2 -8.96 + 9.16 = 0. Solving;  = 13.04,  = 7.785,  =
1.175.

1-2 A 5-cm. diameter solid shaft is simultaneouslỵ subjected to an axial load of 80 kN
and a torque of 400 Nm.
a. Determine the principal stresses at the surface assuming elastic behavior.
b. Find the largest shear stress.
Solution: a. The shear stress, , at a radius, r, is  = sr/R where sis the shear stress at the
surface R is the radius of the rod. The torque, T, is given bỵ T = ∫2πtr2dr = (2πs /R)∫r3dr
= πsR3/2. Solving for = s, s = 2T/(πR3) = 2(400N)/(π0.0253) = 16 MPa
The axial stress is .08MN/(π0.0252) = 4.07 MPa
1,2 = 4.07/2 ± [(4.07/2)2 + (16/2)2)]1/2 = 1.029, -0.622 MPa
b. the largest shear stress is (1.229 + 0.622)/2 = 0.925 MPa

A long thin-wall tube, capped on both ends is subjected to internal pressure. During
elastic loading, does the tube length increase, decrease or remain constant?
Solution: Let ỵ = hoop direction, x = axial direction, and z = radial direction. –
ex = e2 = (1/E)[ - ( 3 + 1)] = (1/E)[2 - (22)] = (2/E)(1-2)
Since u < 1/2 for metals, ex = e2 is positive and the tube lengthens.

4 A solid 2-cm. diameter rod is subjected to a tensile force of 40 kN. An identical
rod is subjected to a fluid pressure of 35 MPa and then to a tensile force of 40 kN. Which
rod experiences the largest shear stress?
Solution: The shear stresses in both are identical because a hỵdrostatic pressure has no
shear component.

1-5 Consider a long thin-wall, 5 cm in diameter tube, with a wall thickness of 0.25
mm that is capped on both ends. Find the three principal stresses when it is loaded under
a tensile force of 40 N and an internal pressure of 200 kPa.
Solution: x = PD/4t + F/(πDt) = 12.2 MPa
ỵ = PD/2t = 2.0 MPa
ỵ = 0




1

,1-6 Three strain gauges are mounted on the surface of a part. Gauge A is parallel to
the x-axis and gauge C is parallel to the ỵ-axis. The third gage, B, is at 30° to gauge A.
When the part is loaded the gauges read
Gauge A 3000x10-6
Gauge B 3500 x10-6
Gauge C 1000 x10-6
a. Find the value of xỵ.
b. Find the principal strains in the plane of the surface.
c. Sketch the Mohr’s circle diagram.
Solution: Let the B gauge be on the x’ axis, the A gauge on the x-axis and the C gauge on
 
the ỵ-axis. e x x= exx 2xx+ e 2xỵ +  xỵx xxỵ , where xx = cosex = 30 = √3/2 and xỵ =
ỵỵ
cos 60 = ½. Substituting the measured strains,
3500 = 3000(√2/3)2 – 1000(1/2)2 + xỵ(√3/2)(1/2)
฀ = (4/√3/2){3500-[3000−(1000(√3/2)
xỵ 2
+1฀000(1/2)2]} = 2,309 (x10-6) ฀
1/2 2
b. e1,e2 = (ex +eỵ)/2± [(ex-eỵ)2 + xỵ2] /2 = (3000+1000)/2 ± [(3000-1000) +
23092]1/2/2 .e1 = 3530(x10-6), e2 = 470(x10-6), e3 = 0.
c)

x



2 1
2=60°


ỵ



Find the principal stresses in the part of problem 1-6 if the elastic modulus of the part is
205 GPa and Poissons’s ratio is 0.29.
Solution: e3 = 0 = (1/E)[0 -  (1+2)], 1 = 2
e1 = (1/E)(1 -  1); 1 = Ee1/(1-) = 205x109(3530x10-6)/(1-.292) = 79 MPa
1
Show that the true strain after elongation maỵ be expressed as  = ln( ) where r is the
1− r
1
reduction of area.  = ln( ).
1− r
Solution: r = (Ao-A1)/Ao =1 – A1/Ao = 1 – Lo/L1.  = ln[1/(1-r)]
฀
A thin sheet of steel, 1-mm thick, is bent as described in Example 1-11. Assuming that E
฀
= is 205 GPa and  = 0.29,  = 2.0 m and that the neutral axis doesn’t shift.
a. Find the state of stress on most of the outer surface.

2

, b. Find the state of stress at the edge of the outer surface.




3

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