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Work done by an external force:Calculate the work done :
1) By gravity on a point mass(m) free falling a distance D under gravity (g)2) By gravity on a point mass(m) pulled vertically up by a distance D.3) By gravity on a car (m) travelling a distance (L) on an uphill slope(q).4) By gravity on a car (m) travelling a distance (L) on a downhill slope(q).
Work done by an External force:Calculate the work done :
1) By force ‘P’ on a massless spring extending (DlP) under load ‘P.’
2) By force ‘P’ on a massless spring extending (DlQ) under additional load ‘Q’, while ‘P’ was already acting.
3) By moment ‘M1’ on a rotational spring rotating (Dq1) under moment ‘M1’.
4) By moment ‘M1’ on a rotational spring rotating (Dq2) under moment ‘M2’, while ‘M1’ was already acting.
5) By a Moment ‘M’ on a beam deforming by (D), rotating by (q).
3
D
q
Work done by an Internal forces (Strain Energy):
Strain Energy (U) is the potential energy that is stored when solid elements undergo deformations.
Axial load ‘P’ is applied gradually to the bar:
Energy (dU) stored in length dx = e.dx. P/2
e= P/AE; therefore, dU = (P2/2AE)(dx)
U= P2L/2AE
Bending Moment M(x) is acting on a beam due to a set of gradually applied loads:
dq = (M/EI)dx
dU= M (d )q /2 = M2(dx)/2EI
U = 4
PD
LA, Edx
P
x
dx
dq
MM
Principle of Work and Energy:Internal Work (Strain Energy) = External WorkU = W =
=
=
U=W
D=
5
D
q
w
-PL
x
L
Principle of Work and Energy:Internal Work (Strain Energy) = External WorkU = W =
=
For more than one point load, we need more than one unknown variables to calculate W. But we have only one equation (W=U). This method is not suitable
6
D
q
M=-wL2/2
x
w
Principle of Virtual Work (Johann Bernoulli, 1717):
• Calculate the forces in each element due to the applied real loads.
• Calculate internal deformations in each element due to the applied real loads (dL).
• Apply a unit virtual load at the location (and direction) where we want to calculate the deformations due to the real loads.
• Calculate internal forces in each element due to the virtual load (u).
• External work by the virtual load while real loads are applied gradually = 1 . D
• Internal work by the virtual load while real loads are applied gradually = ∑u.dL
• 1 . = D ∑u.dL
• Therefore, = D ∑u.dL
Similarly, we can apply unit virtual moment to calculate
• q=∑uq.dL7
Not to be confused with Daniel Bernoulli, though they were contemporaries