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Rigid body - Statics, Diapositivas de Física Clásica

Notes provided for the General Physics course, freshman. Condensed with formulae, excelent as a sum up when memorizing or remembering the main concepts.

Tipo: Diapositivas

2019/2020

Subido el 11/10/2025

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Physics FST - EHU
5b- RIGID BODY
Statics
Physics FST - EHU
Book Chapter
P.A. Tipler, G. Mosca. Physics for Scientists and Engineers.
6th ed., W.H. Freeman & Co Ltd, 2007. 12
H.D. Young, R.A. Freedman, F. Sears, M. Zemansky.
University Physics with Modern Physics. Global Edition (14th
ed.), Pearson Education, 2015.
11
W. Bauer, G.D. Westfall, University Physics with Modern
Physics. McGraw-Hill Global Education, 2011. 11
P.M. Fishbane, S. Gasiorowicz, S.T. Thornton, Fisika
zientzialari eta ingeniarientzat. UPV/EHU-ko argitalpen
zerbitzua, 2008.
11
UEUko Fisika Saila. Fisika Orokorra. UEU, 1992. 10
UEUko Fisika Saila. Fisika Orokorra: Ariketak. UEU, 1989. 11
Bibliography
The contents that will be worked on this topic can be found in the following
book chapters:
Some images appearing in the current document were taken from these
bibliographic sources.
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Physics FST - EHU^1

5b- RIGID BODY

Statics

Physics FST - EHU

Book Chapter

P.A. Tipler, G. Mosca. Physics for Scientists and Engineers.

6th ed., W.H. Freeman & Co Ltd, 2007.

12

H.D. Young, R.A. Freedman, F. Sears, M. Zemansky.

University Physics with Modern Physics. Global Edition (14th

ed.), Pearson Education, 2015.

11

W. Bauer, G.D. Westfall, University Physics with Modern

Physics. McGraw-Hill Global Education, 2011.

11

P.M. Fishbane, S. Gasiorowicz, S.T. Thornton, Fisika

zientzialari eta ingeniarientzat. UPV/EHU-ko argitalpen

zerbitzua, 2008.

11

UEUko Fisika Saila. Fisika Orokorra. UEU, 1992. (^10)

UEUko Fisika Saila. Fisika Orokorra: Ariketak. UEU, 1989. 11

Bibliography

The contents that will be worked on this topic can be found in the following

book chapters:

Some images appearing in the current document were taken from these

bibliographic sources.

Physics FST - EHU^3

Σ

⃗ F ext

= 0 ⃗a CM

= 0

Σ

⃗ M ext

= 0 α⃗ = 0

As a consequence of the external forces acting on a rigid body:

  1. The net force, i.e. sum of all vectors, causes an acceleration of the CM

(independently of the application point of the force):

  1. Depending on the application point of the forces, these may have a

torque that will produce the rotational motion of the body:

Σ

⃗ F ext

=M ⃗a CM

 M = I 

A rigid body will be in STATIC EQUILIBRIUM if and only if:

and ...

The torque depends on the origin used for calculating it, but ...

STATIC EQUILIBRIUM

Physics FST - EHU 4

It will be demonstrated that

If holds with respect to a particular point, i.e. the origin, and the

body is in static equilibrium , it will also hold with respect to any other point.

Σ

⃗ M ext

= 0

x

x '

y '

y

r i

0

0 '

r i

'

 D

x

x '

y '

y

r i

0

0 '

r i

'

 D

M

0

i

 r i

F

i

If it holds with respect to 0 : =^0

When the point of reference changes ( 0' ):

r i

=r i

' 

 D

x

y

r i

00

M

0

i

 r i

F

i

i

r i

D∧

F

i

i

r i

F

i

i

D∧

F

i

i

r i

F

i

D∧

i

F

i

i

r i

F

i

M

0 '

0

**The weight acts as if it was applied on the CM.

Exercises: All