What is the mass of the counterweight in a two-leaf bascule bridge?

  • Thread starter Thread starter lofty28
  • Start date Start date
  • Tags Tags
    Bridges
Click For Summary

Discussion Overview

The discussion revolves around the calculation of the mass of the counterweight in a two-leaf bascule bridge, utilizing principles of torque and equilibrium. Participants explore the mechanics involved in balancing the bridge's leaves and the implications of static friction in a related scenario.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Homework-related

Main Points Raised

  • One participant describes the setup of a two-leaf bascule bridge and provides specific measurements and mass for calculations.
  • Another participant likens the problem to a see-saw, suggesting a simplified analogy to understand the balance of forces.
  • A participant presents a torque equation to calculate the counterweight's mass, showing the steps involved in the calculation.
  • Further clarification is provided on the torque equation, with a suggestion to simplify the expression for clarity.
  • A new question is introduced regarding the lifting of a leaf with a truck on it, focusing on the angle at which the truck would begin to roll back due to static friction.
  • Participants discuss the need for a free body diagram to analyze the forces acting on the truck in the context of the new question.
  • One participant notes the absence of mass information for the truck and suggests using a variable to represent it, indicating that it may cancel out in the calculations.

Areas of Agreement / Disagreement

Participants generally agree on the approach to calculating the counterweight's mass using torque principles, but the discussion introduces a new question about static friction that remains unresolved. There is no consensus on the latter question as it involves additional assumptions and calculations.

Contextual Notes

The discussion includes assumptions about equilibrium and the simplification of forces, which may not be fully explored. The second question introduces additional complexity regarding friction without providing all necessary parameters.

lofty28
Messages
9
Reaction score
0
Modern day draw bridges are also known as bascule bridges. These can have one or two sides (one is called a leaf) that are drawn up from each end of the bridge so that boats can pass through water channels. In some designs, each side of the bascule bridge is held in place by a counter-weight located in a pier placed on the river bank. Imagine one side of a two-leaf bascule bridge. The length of one leaf of the bascule bridge is 25m (from pivot point on the pier to the edge of the leaf that meets the opposite leaf in the middle of the river). The mass of the leaf is 10 000 kg. If the counter weight is located one metre on the other side of the pivot point, use your knowledge of torque (moment of force) to determine the mass of the counterweight. (Hint: The mass of the leaf should be taken from the centre of the leaf and we assume the leaf is at equilibrium in the down position).

I am completely stumped.

Please help!

Thanks
 
Physics news on Phys.org
welcome to pf!

hi lofty28! welcome to pf! :smile:

it's exactly like a see-saw (a teeter-totter) …

how much does the fat kid have to weigh? :biggrin:
 
Would I be right to say...
(f1*L)+(F2*L2)+(F3*L3)=0 (0*25)+(10,000*12.5)+(x * -1)=0 (0)+(125,000)+(x * -1)=0 (125,000)= -(x * -1) 125,000/1 = -x * 1 /1 125,000 = -x
 
hi lofty28! :smile:

let's put some line-breaks in there :rolleyes:
lofty28 said:
(f1*L)+(F2*L2)+(F3*L3)=0

(0*25)+(10,000*12.5)+(x * -1)=0

(0)+(125,000)+(x * -1)=0

(125,000)= -(x * -1)

125,000/1 = -x * 1 /1

125,000 = -x

yes, that's correct until it should be …

(125,000)= -(x * -1)

125,000/1 = x * 1 /1

125,000 = x​

but why not just say "10,000*12.5 = x*1, so x = 125,000"? :wink:
 
Thank you soo much IOU :D

I do have just one more question which relates to the last one...

The bridge from problem 3 needs to draw up the leaves to let a ship through. The leaves are being lifted when someone notices a truck has broken down on one leaf and cannot be moved. It takes some time to stop the motor that controls the lift of the leaf. By how much can the truck be lifted by the leaf of the bridge before it starts to roll back? Assume the coefficient of static friction between the leaf surface and truck is 0.2. In your answer report the angle of the leaf of the bridge at the point just before the truck will roll. When justifying your answer use a free body diagram and appropriate working.

Thanks
 
lofty28 said:
I do have just one more question which relates to the last one...

When justifying your answer use a free body diagram and appropriate working.

this has nothing to do with the last question, this is a simple friction question!

describe (or post an image of) your free body diagram for (only) the truck :smile:
 
I think what the question is asking is at what slope (degree) would the truck start moving backwards?
So I assume that some sort of friction equation would solve this.
All the information we were given is what I posted befor... I know how to find it if the mass was given but it is not given..
 
lofty28 said:
... I know how to find it if the mass was given but it is not given..

ah!

standard trick …

call the mass "m", you'll find it will cancel out in the end! :-p

what do you get? :smile:
 

Similar threads

  • · Replies 7 ·
Replies
7
Views
3K
Replies
1
Views
2K
  • · Replies 11 ·
Replies
11
Views
5K
  • · Replies 2 ·
Replies
2
Views
4K
  • · Replies 2 ·
Replies
2
Views
4K
  • · Replies 1 ·
Replies
1
Views
2K
Replies
1
Views
3K
  • · Replies 31 ·
2
Replies
31
Views
3K
  • · Replies 26 ·
Replies
26
Views
5K
  • · Replies 1 ·
Replies
1
Views
8K