Moment of uniformly distributed load

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Homework Help Overview

The discussion revolves around the calculation of moments due to a uniformly distributed load applied to a beam, specifically at a point labeled R2. Participants are examining the effects of the load's distribution and its position relative to R2.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the calculation of moments at R2, questioning whether the moment due to the distributed load is being correctly interpreted. There are discussions about the positioning of the load and its effect on the moment calculation.

Discussion Status

Some participants have provided insights into the nature of the distributed load and its impact on the moment around R2. There appears to be a productive exchange of ideas, with multiple interpretations being explored regarding the load's placement and its contribution to the moment.

Contextual Notes

There is mention of a diagram that may clarify the load's distribution, but its details are not provided in the text. Participants are also addressing potential misunderstandings about the relationship between the load's total force and its position relative to R2.

chetzread
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Homework Statement



at R2 , is the moment wrong ? it should be 6R1 -200(2)(1) =1800 , am i right ?

Homework Equations

The Attempt at a Solution


it's 200(2)(1) because the uniformly distributed load is from 2m away from R2 , so force should be 200(2) ??
 

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chetzread said:

Homework Statement



at R2 , is the moment wrong ? it should be 6R1 -200(2)(1) =1800 , am i right ?

Homework Equations

The Attempt at a Solution


it's 200(2)(1) because the uniformly distributed load is from 2m away from R2 , so force should be 200(2) ??
Maybe I'm missing something, but it looks to me like the 200 N/m distributed load is centered right smack on R2. In other words, half of that load is to the left of R2, and half to the right: It's distributed evenly spanning 2 m on either side of R2. So the moment around R2 isn't affected by the distributed load (hence the 0 in the "200(4)(0)" term in the attached solution section).
 
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collinsmark said:
Maybe I'm missing something, but it looks to me like the 200 N/m distributed load is centered right smack on R2. In other words, half of that load is to the left of R2, and half to the right: It's distributed evenly spanning 2 m on either side of R2. So the moment around R2 isn't affected by the distributed load (hence the 0 in the "200(4)(0)" term in the attached solution section).
we know that force = wx , where w = force per meter , x = distance , so , do you mean , the x of distributed load start from 0 at R2 , and it is measured from R2 to the left and to the right ...If so , then , it should be 200(2)(1) . am i right ?
 

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chetzread said:
we know that force = wx , where w = force per meter , x = distance , so , do you mean , the x of distributed load start from 0 at R2 , and it is measured from R2 to the left and to the right ...If so , then , it should be 200(2)(1) . am i right ?
There still seems to be a misunderstanding somewhere.

The distributed load is depicted as 200 N/m, and it spans a total of 4 meters. So the total force of the distributed load is 200(4) = 800 N.

This 800 N force is centered directly on top of R2. In other words, it is 0 m from R2. So it's contribution to the total moment around R2 is 200(4)(0) = 0 N⋅m.

If you wanted to break up the distributed load into two forces, each centered 1 m away from R2 on either side, and each spanning 2 meters, you still get the same answer. In that case, one moment will act counterclockwise around R2 and the other clockwise around R2, so the terms will cancel.
200(2)(1) - 200(2)(1) = 0 N⋅m.

[Edited a pair of typos immediately after posting.]
 
collinsmark said:
There still seems to be a misunderstanding somewhere.

The distributed load is depicted as 200 N/m, and it spans a total of 4 meters. So the total force of the distributed load is 200(4) = 800 N.

This 800 N force is centered directly on top of R2. In other words, it is 0 m from R2. So it's contribution to the total moment around R2 is 200(4)(0) = 0 N⋅m.

If you wanted to break up the distributed load into two forces, each centered 1 m away from R2 on either side, and each spanning 2 meters, you still get the same answer. In that case, one moment will act counterclockwise around R2 and the other clockwise around R2, so the terms will cancel.
200(2)(1) - 200(2)(1) = 0 N⋅m.

[Edited a pair of typos immediately after posting.]
i can't understand the 800N is at 2m away from R2 , (either at the left of R2 or right of the R2 ) , am i right ? how could 800N at the center of R2 ? (refer to the diagram)
 

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chetzread said:
i can't understand the 800N is at 2m away from R2 , (either at the left of R2 or right of the R2 ) , am i right ? how could 800N at the center of R2 ? (refer to the diagram)
If you want to balance a cube* with 4 meter sides (such that one of its planes is parallel with the ground) you would find the center of balance (i.e., center of gravity) to be in the middle, correct? If you place the cube on the ground (such that one of its planes is flush with the horizontal ground), the center of force of the cube on the ground is going to be in the middle of that 4 m span, not at one of its sides.

*(assume the cube has uniformly distributed mass)

Does that make sense?
 
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chetzread said:
w = force per meter

You're mixing a physical quantity with a unit of measure.
You may have force divided by distance, or Newtons per metre.
 

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