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Mechanics Tutorial 5 Bridges Monday, 25 February 2019

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1 Mechanics Tutorial 5 Bridges Monday, 25 February 2019
Leeds City College

2 Bridges The simplest bridge is a uniform plank that crosses a space between two supports. We use the principle of moments to work out the forces that act on each support. mg Monday, 25 February 2019 Leeds City College

3 Moments are involved… 2d mg Fucking Hell! Monday, 25 February 2019
Leeds City College

4 Moments on a bridge A B mg
There is a clockwise moment about A, and an anti-clockwise moment about B Clockwise Moment = mg × d Anticlockwise moment = mg × d Since force = moment ÷ distance, the force on each pivot, A and B, is given by: F = mg/2 mg A B 2d Monday, 25 February 2019 Leeds City College

5 Putting a load on a bridge
mg A B 2d m1 m1g x The centre of mass is in the same place, but we now have an extra load of m1g on the bridge. Force on A = moment about B ÷ distance between A and B Taking moments about B: Force on A = Moment about B ÷ 2d = (mg × d) + (m1g × x) 2d Moment = (mg × d) + (m1g × x) Force on B = moment about A ÷ 2d = (mg × d) + (m1g × [2d – x]) 2d Taking moments about A: Moment = (mg × d) + (m1g × [2d – x]) Monday, 25 February 2019 Leeds City College

6 Ladder S A ladder can be treated using moments
The ladder is stable because all four faces form a closed rectangle F is the friction to hold the ladder against the wall. Length, l Normal force, N W = mg q F A Monday, 25 February 2019 Leeds City College

7 Ladder B S We can resolve vertically and horizontally: N = W and S = F
Anti-clockwise moment about A = S × l sin q Length, l Clockwise moment about A = W × l/2 cos q Normal force, N Principle of moments: S × l sin q = W × (l/2) cos q W = mg Therefore: q F A Monday, 25 February 2019 Leeds City College


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