University of Florida/Egm3520/s13.team4.r2

Report 2

Problem 2.1

Pb-9.1 in sec.9.

Indented line

Problem Statement

1)Solve for the reactions at B and at A in the Example 2.04 (see textbook page 72) with the stress strain relation $\sigma =E{ϵ}^{1/2}$
2)Do the results depend on the length of each segment and the Young's modulus?

Solution

problem 2.04, Beer 2012 p.72

Given:

Length

$L_{AD}=L_{DC}=L=150mm$

$L_{CK}=L_{KB}=L=150mm$

Area

$A_{AD}=A_{DC}=A_{AC}=250m{m}^2$

$A_{CK}=A_{KB}=A_{CB}=400m{m}^2$

Young's modulus

$E_{AD}=E_{DC}=E_{CK}=E_{KB}=E$

Applied forces

$F_D=300kN$

$F_K=600kN$

Draw a Free Body Diagram for each section

2.04 problem, Vu-Quoc sec.9 p.9-6

Use $\sum 𝐅\mathbf{=}\mathrm{𝟎}$ on FBD 3

$P_{CK}=R_B-F_K$

Knowing that the strain relation is found by:

$\delta =ϵL=\frac{{\sigma }^2}{E^2}L=\frac{P^{2}L}{A^2{E}^2}$

We understand that without a linear strain relation we can't use the superposition principle to separate the reaction as we did in class.
So we'll need to set two FBD's displacement equations equal to each other in order to solve


The displacement equation mentioned previously is applied to FBD 3, which yeilds:

${\delta }_{CK}=-\frac{P_{CK}^2{L}_{CK}}{(A_{CK}{)}^2(E_{CK}{)}^2}=-\frac{(R_B-F_K{)}^{2}L}{(A_{CB}{)}^2{E}^2}$

To solve for $R_B$ we must sum all displacements from each section we cut and set it equal to 0

These equations yield

${\delta }_{AD}=\frac{(R_B-F_K-F_D{)}^{2}L}{(250{)}^2{E}^2}$

${\delta }_{DC}=\frac{(R_B-F_K{)}^{2}L}{(250{)}^2{E}^2}$

${\delta }_{CK}=\frac{(R_B-F_K{)}^{2}L}{(400{)}^2{E}^2}$

${\delta }_{KB}=\frac{(R_B{)}^{2}L}{(400{)}^2{E}^2}$

${\delta }_T=\sum \delta =0$

${\delta }_T={\delta }_{AD}+{\delta }_{DC}+{\delta }_{CK}+{\delta }_{KB}=0$

since all quantities are squared, therefore

${\delta }_{AD}=0$

${\delta }_{DC}=0$

${\delta }_{CK}=0$

${\delta }_{KB}=0$

$0=\frac{(R_B-F_K-F_D{)}^{2}L}{(250{)}^2{E}^2}$

$0=\frac{(R_B-F_K{)}^{2}L}{(250{)}^2{E}^2}$

$0=\frac{(R_B-F_K{)}^{2}L}{(400{)}^2{E}^2}$

$0=\frac{(R_B{)}^{2}L}{(400{)}^2{E}^2}$

$R_B=0$

$R_B-F_K=0$

$F_K=0$

$R_B-F_K-F_D=0$

$F_D=0$

Solution 2.04

Problem R2.2

P2.12, Beer 2012

Problem Statement

A nylon thread is to be subjected to a 10-N tension. Knowing that E = 3.2 GPa, that the maximum allowable normal stress is 40 MPa, and that the length of the thread must not increase by more than 1%, determine the required diameter of the thread

Solution

GIVEN:

$P=10N$

$E=3.3GPa$

$\sigma =40MPa$

WE KNOW THAT

$\delta =\frac{PL}{AE}$

AND IT IS REQUIRED THAT

$\delta <0.001L$

$\Rightarrow \frac{PL}{AE}<0.001L$

$\Rightarrow \frac{AE}{P}<100$

$\Rightarrow A>\frac{100P}{E}$

AND WE ALSO KNOW THAT $A=\frac{\pi }{4}\times d^2$

SO $\frac{\pi }{4}\times d^2<\frac{100P}{E}$

$\Rightarrow d^2<\frac{400P}{\pi E}$

$\Rightarrow d>20\sqrt{\frac{p}{\pi E}}$

$\Rightarrow d>20\sqrt{\frac{10}{\pi \times 3.2\times 10^9}}$

$d>0.63mm$

On our honor, we did this assignment on our own, without looking at the solutions in previous semesters or other online solutions.

Problem R2.3

P2.16, Beer 2012

Problem Statement

The brass tube AB (E = 105 GPa) has a cross-sectional area of 140 mm^2 and is fitted with a plug at A. The tube is attached at B to a rigid plate that is itself attached at C to the bottom of an aluminum cylinder (E = 72 GPa) with a cross-sectional area of 250 mm^2. The cylinder is then hung from a support at D. In order to close the cylinder, the plug must move down through 1 mm. Determine the force P that must be applied to the cylinder.

Solution

Given: Brass Tube AB: $E_{AB}=105\ast 10^{9}Pa$

$A_{AB}=140m{m}^2$

$L_{AB}=1+375=376mm$

Aluminum Cylinder DC:

$E_{DC}=72\ast 10^{9}Pa$

$A_{DC}=250m{m}^2$

$L_{DC}=375mm$

Equations: Compression of Brass Tube AB: ${\delta }_{AB}=\frac{P\ast L_{AB}}{A_{AB}\ast E_{AB}}=\frac{(376)P}{(105\ast 10^9)(140)}=(2.56\ast 10^{-}11)\ast P$

Tension of Aluminum Cylinder DC: ${\delta }_{DC}=\frac{P\ast L_{DC}}{A_{DC}\ast E_{DC}}=\frac{(375)P}{(72\ast 10^9)(250)}=(2.1\ast 10^{-}11)\ast P$

We know the total deflection:

${\delta }_T=1mm$

${\delta }_T={\delta }_{AB}+{\delta }_{DC}\Rightarrow 1=(2.56\ast 10^{-}11)P+(2.1\ast 10^{-}11)P=(4.66\ast 10^{-}11)P$

$\Rightarrow P=2.15\ast 10^{1}0mN,or21.5kN$

On our honor, we did this assignment on our own, without looking at the solutions in previous semesters or other online solutions.

Problem R2.4

P2.24, Beer 2012

Problem Statement

For the steel truss (E = 29 x 10^6 psi) and loading shown, determine the deformations of members BD and DE, knowing that their cross-sectional areas are 2 in^2 and 3 in^2, respectively.

Solution

Free Body Diagrams

$\sum F_x=0=-F_x+90kips\Rightarrow F_x=90kips$

$\sum M_F=0=-30kips\ast 16ft-30kips\ast 8ft-24ft\ast 30kips+G_y\ast 15ft\Rightarrow G_y=96kips(tension)$

$\sum F_y=0=F_y+G_y\Rightarrow F_y=-G_y=-96kips$

$\sum F_x=0=-F_x+30kips+F_{DE}\Rightarrow F_{DE}=90kips-30kips=60kips$

$\sum M_G=0=-30kips\ast 8ft+F_y\ast 15ft-F_{BD}\ast 15ft-F_{DE}\ast 8ft\Rightarrow F_{BD}=\frac{60kips\ast 8ft+30kips\ast 8ft-96kips\ast 15ft}{15ft}=-48kips(tension)$

${\delta }_{BD}=\frac{PL}{AE}=\frac{48kips\ast 8ft\ast 12\frac{in}{ft}}{2i{n}^2\ast 29\ast 10^3\frac{kips}{i{n}^2}}=0.0794in$

${\delta }_{DE}=\frac{PL}{AE}=\frac{60kips\ast 15ft\ast 12\frac{in}{ft}}{3i{n}^2\ast 29\ast 10^3\frac{kips}{i{n}^2}}=0.124in$

On our honor, we did this assignment on our own, without looking at the solutions in previous semesters or other online solutions.

Problem R2.5

P2.40, Beer 2012

Problem Statement

A polystyrene rod consisting of two cylindrical portions AB and BC is restrained at both ends and supports two 6-kip loads as shown. Knowing that E = 0.45 X 10^6 psi, determine (a) the reactions at A and C, (b) the normal stress in each portion of the rod.

Solution

Splitting the diagram into two parts we get part 1 and part 2 So we are given:

Part 1:

$d_1=1.25in$

$L_1=25in$

Part 2:

$d_2=2in$

$L_2=15in$

$E=0.45\times 10^{6}psi$

$A_1=\frac{\pi d_1^2}{4}=1.227i{n}^2$

$A_2=\frac{\pi d_2^2}{4}=3.14i{n}^2$

Looking at the free body diagram we see that

$R_1+R_2=12kip$

The total ${\delta }_{total}$ equals zero so

${\delta }_{total}=0={\delta }_1+{\delta }_2$

Using the formula

$\delta =\frac{PL}{AE}$

We find that

$\frac{P_1{L}_1}{A_1{E}_1}+\frac{P_2{L}_2}{A_2{E}_2}=0$

Substituting in the reaction forces $R_1$ and $R_2$

$(R_2$ will show negative because the force is facing opposite to $R_1)$

$\frac{R_1{L}_1}{A_1{E}_1}-\frac{R_2{L}_2}{A_2{E}_2}=0$

Solving for $R_1$ we get

$R_1=\frac{R_2{A}_1{L}_2}{L_1{A}_2}$

So

$R_1=.2344R_2\mathrm{....}(1)$ and solving a system of equations with

$R_1+R_2=12kip\mathrm{....}(2)$ Gives

$R_1=2.27kips$
$R_2=9.72kips$

(b) Using the formula $\sigma =\frac{P}{A}$

So

${\sigma }_1=\frac{R_1}{A_1}=1.85ksi$
${\sigma }_2=\frac{R_2}{A_2}=3.09ksi$

On our honor, we did this assignment on our own, without looking at the solutions in previous semesters or other online solutions.

Problem R2.6

P2.44, Beer 2012

Problem Statement

The rigid bar AD is supported by two steel wires of 1 16-in. diameter (E = 29 X 10^6 psi) and a pin and bracket at D. Knowing that the wires were initially taut, determine (a) the additional tension in each wire when a 120-lb load P is applied at B, (b) the corresponding deflection of point B.

Solution

${\delta }_{AE}=\frac{P_{AE}{L}_{AE}}{AE}$

$\Rightarrow P_{AE}=\frac{{\delta }_{AE}\ast AE}{L_{AE}}=\frac{24in\ast \theta \ast \frac{\pi }{4}\ast (\frac{1}{16}in{)}^2\ast 29\ast 10^{6}psi}{15in}=142.4kips\ast \theta$

${\delta }_{CF}=\frac{P_{CF}\ast L_{CF}}{AE}$

$\Rightarrow P_{CF}=\frac{{\delta }_{CF}AE}{L_{CF}}=\frac{8in\ast \frac{\pi }{4}\ast (\frac{1}{16}in{)}^2\ast 29\ast 10^{6}psi}{8in}=88.97kips\ast \theta$

$\sum M_D=0=-24in\ast P_{AE}+16in\ast P-8in\ast P_{CF}=-24in\ast 142.4\ast 10^{3}lb\ast \theta +16in\ast 120lb-8in\ast 88.97\ast 10^{3}lb\ast \theta$

$\Rightarrow \theta =465\ast 10^{-6}$

$P_{AE}=142.4\ast 10^{3}lb\ast 465\ast 10^{-6}=66.21lb$

$P_{CF}=88.97\ast 10^{3}lb\ast 465\ast 10^{-6}=41.37lb$

${\delta }_B=16in\ast \theta =16in\ast 465\ast 10^{-6}=7.44\ast 10^{-3}(downward)$

On our honor, we did this assignment on our own, without looking at the solutions in previous semesters or other online solutions.