background image

 

 

 

 

Project “The development of the didactic potential of Cracow University of Technology in the range of modern 

construction” is co-financed by the European Union within the confines of the European Social Fund  

and realized under surveillance of Ministry of Science and Higher Education. 

1

Exercise 4.2  
 
For a given planar force system find: 
 
I

           An equivalent coupe-force system at point  A.  

II. 

The simplest equivalent force system. Draw the result of reduction on the figure. 

 

                                  
            
 
 
 
 
 
 
 
 
 
 
 
 

 

q

1

=4 kN/m

17 kNm

q

2

=

kN/m

14 kN

10 kN

15 kN

3

2 kN

2m

4m

1m

2m

=3 kN/m2

A

x

y

 
 
 
The origin of the coordinate system is positioned at point A 
 

I.  An equivalent couple-force system at point A 
 

  Replacing  the distributed loads by their resultants. 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 

 

q

1

=4 kN/m

M

1

=17 kNm

q

2

=

kN/m

F

4

=14 kN

F

1

=10 kN

15 kN

3

2 kN

2m

4m

1m

2m

=3 kN/m2

A

x

y

F

6

F

5

W

1

W

2

2
3

*l

2

1
3

*l

2

W

3

F

2

F

3

1

l

2

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construction” is co-financed by the European Union within the confines of the European Social Fund  

and realized under surveillance of Ministry of Science and Higher Education. 

2

 

])

[

4

],

/

[

4

(

1

1

1

1

1

m

l

m

kN

q

l

q

W

 

]

[

16

]

[

4

]

/

[

4

1

kN

m

m

kN

W

 

 

])

3

[

],

/

[

2

(

2

1

2

2

2

2

2

m

l

m

kN

q

l

q

W

 

]

[

3

]

[

3

]

/

[

2

2

1

2

kN

m

m

kN

W

 

 

])

[

2

]

[

2

]

[

1

],

/

[

3

(

2

2

3

m

m

m

area

m

kN

area

W

 

]

[

6

]

[

2

]

/

[

3

2

2

3

kN

m

m

kN

W

 

 

  Resolving the oblique forces into components 
  

]

[

2

3

)

45

sin(

2

kN

F

]

[

2

3

)

45

cos(

3

kN

F

 

]

[

3

3

2

kN

F

F

 

Where: 

5

4

)

cos(

5

3

)

sin(

(see the figure) 

]

[

12

]

[

15

)

cos(

5

kN

kN

F

 

]

[

9

]

[

15

)

sin(

6

kN

kN

F

 

  Determining the sum vector 

)

,

,

(

O

S

S

S

y

x

 

2

5

2

1

W

F

F

F

S

x

 

 

 

]

[

kN

S

x

3

1

6

4

3

W

W

F

F

F

S

y

      

                     

]

[

kN

S

y

)

],

[

2

],

[

2

(

O

kN

kN

S

 

 

  Detrmining the total moment about point A 

 

Project “The development of the didactic potential of Cracow University of Technology in the range of modern 

 
 

 
 
 
 
 
 
 
 
 
 
 
 
 
 

M

1

F

4

F

1

2m

2m

1m

2m

A

x

y

F

6

F

5

W

1

W

2

W

3

F

2

F

3

r

F1

r

F3

r

F5

r

F6

r

W3

r

W1

2m

r

W2

+

-

1m

2m

background image

 

 

 

 

Project “The development of the didactic potential of Cracow University of Technology in the range of modern 

construction” is co-financed by the European Union within the confines of the European Social Fund  

and realized under surveillance of Ministry of Science and Higher Education. 

3

 

)

,

0

,

0

(

Az

A

M

M

 (for a planar force system) 

1

3

3

2

2

1

1

6

6

5

5

3

3

1

1

M

r

W

r

W

r

W

r

F

r

F

r

F

r

F

M

W

W

W

F

F

F

F

Az

 

 

Remark: the moment of  F

2

 and  F

4

 about A equal zero,  because their lines of action pass through that point. 

 

]

[

4

]

[

17

]

[

1

]

[

6

]

[

1

]

[

3

]

[

2

]

[

16

]

[

4

]

[

9

]

[

2

]

[

12

]

[

2

]

[

3

]

[

1

]

[

10

kNm

kNm

m

kN

m

kN

m

kN

m

kN

m

kN

m

kN

m

kN

M

Az

 

])

[

4

,

0

,

0

(

kNm

M

A

 

 

  Answer  
The planar system of forces can be reduced at point A to a coupe-force system comprising one force  

)

],

[

2

],

[

2

(

O

kN

kN

S

 applied at point A, and one couple with a moment 

])

[

4

,

0

,

0

(

kNm

M

A

 
 

II.  The simplest equivalent system 

 

 

)

],

[

2

],

[

2

(

O

kN

kN

S

])

[

4

,

0

,

0

(

kNm

M

A

 hence the parameter of the system  

0

A

M

S

k

 

 

             

0

0

k

S

 the system can be reduced to a resultant force. 

 
 

  The equation of a central axis 

0

);

,

,

(

P

M

z

y

x

P

 

 

P

A

S

M

M

A

p

  

)

0

,

,

(

)

0

,

,

(

int

)

0

,

0

,

0

(

int

y

x

P

A

vector

y

x

P

po

A

po

  

)

0

,

,

(

)

0

],

[

2

],

[

2

(

y

x

P

A

kN

kN

S

 

)

]

[

2

]

[

2

,

0

,

0

(

x

kN

y

kN

P

A

S

 

P

A

S

M

A

0

 

 

)

]

[

2

]

[

2

,

0

,

0

(

])

[

4

,

0

,

0

(

)

0

,

0

,

0

(

x

kN

y

kN

kNm

[

2

]

[

2

]

[

2

]

[

4

0

m

x

y

x

kN

y

kN

kNm

]

 

 
 

]

[

m

x

y

   the central axis (or the line of action of the resultant force.)

 

 

  Answer  

The given  planar system of forces  can be reduced to a resultant force  equal to the sum vector, acting along the 
central 

 

]

[

m

x

y

 
 
 
 
 
 
 

background image

 

 

 

 

Project “The development of the didactic potential of Cracow University of Technology in the range of modern 

construction” is co-financed by the European Union within the confines of the European Social Fund  

and realized under surveillance of Ministry of Science and Higher Education. 

4

 
 
 

q

1

=4 kN/m

17 kNm

q

2

=

2 kN/m

14 kN

10 kN

15 kN

3

2 kN

2m

4m

1m

2m

=3 kN/m2

A

x

y

y=

x-

2[

m

]

W=S(-2[kN ],-2[kN ])