01.11.2021 Views

Timothy A. Philpot - Mechanics of materials _ an integrated learning system-John Wiley (2017)

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

ExAmpLE 17.14

1,400 N

900 N

Calculate the deflection at end C of the cantilever beam shown.

Assume that E = 70 GPa for the entire beam.

A

I = 160,000 mm 4

B

I = 20,000 mm 4 C

300 mm 165 mm

C

1 N

Plan the Solution

For the cantilever beam considered here, the virtual-moment equation

will be continuous over the entire span, but the real-moment

equation is discontinuous at B. Therefore, the beam must be considered

in two segments: AB and BC. The moment equations will be

simpler to derive if the origin of the x coordinate system is placed

at the free end C.

A

m

B

x

300 mm 165 mm

1 N

SolutioN

Virtual Moment m: Remove the real loads from the beam and

apply a virtual unit load downward at C, where the deflection is

desired. At this stage of the calculation, it makes no difference that

the beam depth changes along the span, since only the virtual

moment m is needed here.

Now draw a free-body diagram around end C of the beam.

Place the origin of the x coordinate system at C. From the free-body

diagram, derive the following equation for the virtual internal

moment m:

v

x

C

m =−(1 N) x 0 ≤ x ≤ 465 mm

M

900 N

Real Moment M: Remove the virtual load, and reapply the real loads at B and

C. Draw a free-body diagram around end C that cuts through segment BC of the

beam. The same x coordinate used to derive the virtual moment must be used to

derive the real moment; therefore, the origin of the x coordinate system must be

placed at C. From the free-body diagram, derive the following equations for the

real internal moment M:

V

x

C

M =−(900 N) x 0 ≤ x ≤ 165 mm

Now draw a second free-body diagram that cuts through segment AB of the

beam and includes the free end of the cantilever. From the free-body diagram,

derive the following equations for the real internal moment M:

M

1,400 N

900 N

M =−(1,400 N)( x −165 mm) − (900 N) x

=− (2,300 N) x + (1,400 N)(165 mm)

165 mm < x ≤ 465 mm

V

B

x

165 mm

C

The moment of inertia differs for segments AB and BC. This difference will

be incorporated into the calculation in the term M/EI. The equations developed

so far, along with the limits of integration, are conveniently summarized in the

following table:

768

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!