12 MECHANICAL ENGINEERING PRINCIPLES
1.10 Modulus of rigidity
Experiments have shown that under pure torsion (see
Chapter 10), up to the limit of proportionality, we
have Hooke’s law in shear, where
shear stress
shear strain
=rigidity (or shear) modulus
or
τ
γ
=G ( 1. 1 )
whereτ =shear stress,
γ =shear strain (see Figures 1.5 and 1.6) and
G=rigidity (or shear) modulus
1.11 Thermal strain
If a bar of lengthLand coefficient of linear expan-
sion α were subjected to a temperature rise of
T, its length will increase by a distanceαLT,as
described in Chapter 20. Thus the new length of the
bar will be:
L+αLT=L( 1 +αT)
Now, as the original length of the bar wasL,then
thethermal straindue to a temperature rise will be:
ε=
extension
original length
=
αLT
L
i.e. ε=αT
However, if the bar were not constrained, so that
it can expand freely, there will be no thermal
stress.
If, however, the bar were prevented from expand-
ing then there would be a compressive stress in
the bar.
Now ε=
original length−new length
original length
=
L−L( 1 +αT)
L
=
L−L−LαT
L
i.e. ε=−αT
and, since stress =strain×E,then
σ =−αTE
Problem 18. A steel prop is used to
stabilise a building, as shown in Figure 1.11.
(a) If the compressive stress in the bar at
20 °C is 30 MPa, what will be the stress in
the prop if the temperature is raised to
35 °C? (b) At what temperature will the prop
cease to be effective?
TakeE= 2 × 1011 N/m^2 and
α= 14 × 10 −^6 /°C.
Prop
Rigid floor
Building
Figure 1.11
(a) Additional thermal strain,
εT =−αT
=−( 14 × 10 −^6 /°C)×( 35 − 20 )°C
i.e.εT =− 14 × 10 −^6 × 15 =− 210 × 10 −^6
Additional thermal stress,
σT =EεT
= 2 × 1011 N/m^2 ×(− 210 × 10 −^6 )
i.e.σT =−42 MPa
Hence, the stress at 35°C=initial stress+σT
=(− 30 − 42 )MPa
i.e.σ =−72 MPa
(b) For the prop to be ineffective, it will be nec-
essary for the temperature to fall so that there
is no stress in the prop, that is, from 20°C
the temperature must fall so that the initial
stress of 30 MPa is nullified. Hence, drop in
stress=−30 MPa