1. The young's modulus is given by the gradient of a stress-strain graph in its linear region
D2. The force which the cable can support at its breaking point is given by

Therefore the mass is given by
C3. The strain energy of the sample can be estimated by the area under the graph from the origin to the stretched strain value.
B4. It is important for a cable in a crane not to undergo plastic deformation, this sample R would be chosen as it deforms elastically for the greatest range of strain values.
D5. We know that

,

and

From this we can derive the equation
We have;



and from the linear region of the graph for cable R;

A6. The torque about point P is given by the force provided by the mass multipled by the perpendicular distance.
C7. To find the tension in SR we cneed to sum the torques about point P and equate them to zero, as the system is in rotational equilibrium.

C8. To find the force extered by KL downwards on MN we can sum the torques about point K and equate them to zero, as once again this system is in rotational equilibrium.
The additional forces acting are that of the weight of the beam and the mass at point L, these both cause torques.

D9. Personally I don't think any of the options would be appropriate placement of the beams, however, option A is the most appropriate of those given as for the mostpart the top of the beam will be in tension.
A10. It can be noted that the mass at point G will elongate the beam FG, in order to counteract the tension in this beam both EF and FH must be in compression.
B11. The arch is in compression and the weight of the truck on the road will cause the road to deflect downwards and as such the cables will elongate and will be in tension.
B