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Moments At angles.

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1 Moments At angles

2 Starter: Spot the mistake
Moments: At an angle KUS objectives BAT solve problems using moments and friction at angles to a rod/ object using sohCahToa Starter: Spot the mistake

3 Moments The moment of a force measures the turning effect of the force on the body on which it is acting The moment of a force F about a point P is the product of the magnitude of the force and the perpendicular distance of the line of action of the force from the point P Moment of F about P = Fd clockwise The magnitude of the force is measured in newtons (N) and the distance is measured in metres (m), so the moment of the force is measured in newton-metres (Nm) Moment of F about P = 15 Nm anticlockwise

4 Using Trigonometry You may need to use trigonometry to find the perpendicular distance Moment of F about P = clockwise e.g. Moment of the force about P = = clockwise

5 WB 1 Calculate the moment about point A of each of these forces acting on a Lamina ,
𝐴 10 𝑁 40Β° 5 π‘š 𝐴 6 sin 25 5 sin 40 6 π‘š 25Β° 18 𝑁 π‘šπ‘œπ‘šπ‘’π‘›π‘‘=10Γ—5 sin 40=32.1 π‘π‘š π‘Žπ‘π‘€ π‘šπ‘œπ‘šπ‘’π‘›π‘‘=18Γ—6 sin 25=45.6 π‘π‘š π‘Žπ‘π‘€ 𝐴 120 𝑁 50Β° 8 π‘š 70 𝑁 4 sin 65 8 cos 50 𝐴 65Β° 4 π‘š π‘šπ‘œπ‘šπ‘’π‘›π‘‘=70Γ—4 sin 65 =254 π‘π‘š π‘Žπ‘π‘€ π‘šπ‘œπ‘šπ‘’π‘›π‘‘=120Γ—8 cos 50 =617 π‘π‘š 𝑐𝑀

6 WB 2 Given the moment about point A of each of these forces is 20 Nm, Find the magnitude of each force 3 sin 35 𝐴 𝐴 𝐹 1 30Β° 5 π‘š 5 sin 30 3 π‘š 𝐹 2 35Β° 𝐹 2 = 20 3 sin 35 = 𝑁 𝐹 1 = 20 5 sin 30 =8 𝑁 𝐴 75Β° 9 π‘š 𝐹 4 𝐹 3 = 20 2 sin 55 = 𝑁 9 sin 75 𝐴 125Β° 2 π‘š 𝐹 3 2 sin 55 𝐹 4 = 20 9 sin 75 = 𝑁

7 WB 3a Two forces act on a lamina as shown
WB 3a Two forces act on a lamina as shown. Calculate the resultant moment about the point A a) 𝐴 𝐹 2 =5 50Β° 10 π‘š 𝐹 1 =8 30Β° 5 sin 50 8 sin 30 Moment of 𝐹 1 =8 sin 30 Γ—8=32 𝑐𝑀 Moment of 𝐹 2 =5 sin 50 Γ—5= π‘Žπ‘π‘€ Moment of 𝐹 1 and 𝐹 2 =32βˆ’19.2 =12.8 π‘π‘š π‘π‘™π‘œπ‘π‘˜π‘€π‘–π‘ π‘’

8 WB 3b Two forces act on a lamina as shown
WB 3b Two forces act on a lamina as shown. Calculate the resultant moment about the point A b) 𝐴 𝐹 2 =15 60Β° 10 π‘š 𝐹 1 =12 70Β° 8 π‘š 8 sin 60 10 sin 70 Moment of 𝐹 1 =10 sin 70 Γ—12= π‘Žπ‘π‘€ Moment of 𝐹 2 =8 sin 60 Γ—15= 𝑐𝑀 Moment of 𝐹 1 and 𝐹 2 =112.7βˆ’103.9 =8.8 π‘π‘š π‘Žπ‘›π‘‘π‘–π‘π‘™π‘œπ‘π‘˜π‘€π‘–π‘ π‘’

9 Moment on a uniform beam / rod
WB4 review A light rod AB is 4 m long and can rotate in a vertical plane about fixed point C where AC = 1 m. A vertical force F of 7 N acts on the rod downwards. Find the moment of F about C when F acts a) at A b) at B c) at C a) Taking moments about C acw 7 3 m 1 m A C B 8×𝐴𝐢=8 π‘π‘š b) Taking moments about C cw 8×𝐢𝐡=24 π‘π‘š c) Taking moments about C cw 8×𝐢𝐢=0

10 WB 5 The diagram shows a set of forces acting on a uniform rod of mass 3 kg. Calculate the resultant moment about point A (including direction) 𝐴 45Β° 3 π‘š 5 𝑁 6 𝑁 70Β° 4 π‘š 4 sin 45 3 sin 70 Taking moments about A clockwise 6Γ—4 sin 45 βˆ’ 5Γ—3 sin 70 = π‘π‘š π‘π‘™π‘œπ‘π‘˜π‘€π‘–π‘ π‘’

11 Equilibrium

12 WB 6 A uniform rod PQ is hinged at point P, and is held in equilibrium at an angle of 50ο‚° to the horizontal by a force of magnitude F acting perpendicular to the rod at Q. Given that the rod has a length of 3 m and mass of 8 kg, find the value of F 𝑃 8𝑔 𝑁 50Β° 𝐹 𝑄 3 2 cos 50 Taking moments about P 𝐹 Γ—3 = 8𝑔× 3 2 cos 50 𝐹 = 8𝑔× 3 2 cos =25.2 𝑁

13 WB 6 (cont) A uniform rod PQ is hinged at point P, and is held in equilibrium at an angle of 50ο‚° to the horizontal by a force of magnitude F acting perpendicular to the rod at Q. Given that the rod has a length of 3 m and mass of 8 kg, find the value of F 𝑃 8𝑔 𝑁 50Β° 𝐹 𝑄 3 2 cos 50 Taking moments about P 𝐹 Γ—3 = 8𝑔× 3 2 cos 50 𝐹 = 8𝑔× 3 2 cos =25.2 𝑁

14 WB 7 A uniform rod PQ of mass 40 kg and length 10 m rests with the end P on rough horizontal ground. The rod rests against a smooth peg C where AC = 8 m The rod is in limiting equilibrium at an angle of 15ο‚° to the horizontal. Find The magnitude of the reaction at C The coefficient of friction between the rod and the ground 𝑃 40𝑔 15Β° 𝑁 𝐢 𝑅 πΉπ‘Ÿπ‘–π‘π‘‘π‘–π‘œπ‘› 75Β° distance 5 cos 15 a) Taking moments about P 𝑁×8 =40𝑔×5 cos 15 reaction at C 𝑁 = 40𝑔×5 cos = 𝑁 b) Equilibrium in horizontal direction πΉπ‘Ÿπ‘–π‘π‘‘π‘–π‘œπ‘› =𝑁 cos 75 =236.7 cos 75 =61.25 Equilibrium in vertical direction 𝑅+𝑁𝑠𝑖𝑛 75=40𝑔 𝑅=40π‘”βˆ’236.7 cos 75 = 𝑁 πœ‡= πΉπ‘Ÿ 𝑅 = =0.375 Coefficient friction

15 WB 8 A ladder PQ of mass m kg and length 3a m rests with the end P on rough horizontal ground. The other end Q rests against a smooth vertical wall. A load of mass 2m is fixed on the ladder at point C, where AC = a. The ladder is modelled as a uniform rod in a vertical plane perpendicular to the wall and the load as a particle. The ladder rests in limiting equilibrium at an angle of 60ο‚°with the ground. Find the coefficient of friction between the rod and the ground N Add all the forces to the diagram 𝑃 60Β° 𝐢 𝑄 2π‘Ž π‘Ž Wall smooth No friction Equilibrium in horizontal direction πΉπ‘Ÿπ‘–π‘π‘‘π‘–π‘œπ‘›=𝑁 R Equilibrium in vertical direction 𝑅=2π‘šπ‘”+π‘šπ‘”=3π‘šπ‘” Friction

16 (to get an equation with Friction and R)
WB 8 (cont) A ladder PQ of mass m kg and length 3a m rests with the end P on rough horizontal ground. The other end Q rests against a smooth vertical wall. A load of mass 2m is fixed on the ladder at point C, where AC = a. The ladder is modelled as a uniform rod in a vertical plane perpendicular to the wall and the load as a particle. The ladder rests in limiting equilibrium at an angle of 60ο‚°with the ground. Find the coefficient of friction between the rod and the ground Taking moments about Q (to get an equation with Friction and R) 𝑃 60Β° 𝐢 𝑄 2π‘Ž π‘Ž Wall smooth No friction Friction R N 𝑅×3π‘Ž cos 60 =πΉπ‘Ÿπ‘–π‘π‘‘π‘–π‘œπ‘› Γ—3π‘Ž sin 60 +π‘šπ‘”Γ— 3 2 π‘Ž cos 60 +2π‘šπ‘”Γ—2π‘Ž cos 60 Substituting πΉπ‘Ÿπ‘–π‘π‘‘π‘–π‘œπ‘› πœ‡π‘… and R=3π‘šπ‘” 3π‘šπ‘”Γ—3π‘Ž cos 60 =πœ‡3π‘šπ‘” Γ—3π‘Ž sin 60 +π‘šπ‘”Γ— 3 2 π‘Ž cos 60 +2π‘šπ‘”Γ—2π‘Ž cos 60 Cancel by mga and rearrange to πœ‡= 3π‘šπ‘”Γ—3π‘Ž cos 60 βˆ’+π‘šπ‘”Γ— 3 2 π‘Ž cos 60 βˆ’2π‘šπ‘”Γ—2π‘Ž cos 60 3π‘šπ‘” Γ—3π‘Ž sin 60 = cos sin 60 = =0.225

17 WB 9 (exam Q) sin πœƒ = 3 5 cos πœƒ = 4 5 3 4 5 πœƒ Mg 3Mg T R Friction
A plank, AB, of mass M and length 2a, rests with its end A against a rough vertical wall. The plank is held in a horizontal position by a rope. One end of the rope is attached to the plank atΒ B and the other end is attached to the wall at the point C, which is vertically above A. A small block of mass 3M is placed on the plank at the point P, where AP = x The plank is in equilibrium in a vertical plane which is perpendicular to the wall The angle between the rope and the plank is Ξ±, where tan ∝ = 3 4 The plank is modelled as a uniform rod, the block is modelled as a particle and the rope is modelled as a light inextensible string Using the model, show that the tension in the rope is 5𝑀𝑔 3π‘₯+π‘Ž 6π‘Ž sin πœƒ = 3 5 cos πœƒ = 4 5 3 4 5 πœƒ Q from 2018 June exam Mg 3Mg T R Friction

18 WB 9a (exam Q cont ) Using the model, show that the tension in the rope is 5𝑀𝑔 3π‘₯+π‘Ž 6π‘Ž a) Taking moments about A 𝑇 sin ∝ Γ—2π‘Ž =π‘€π‘”Γ—π‘Ž+3𝑀𝑔×π‘₯ Mg 3Mg R Friction a βˆ’π‘‡π‘π‘œπ‘  ∝ 𝑇 sin ∝ Rearranges to 𝑇× 6π‘Ž 5 =π‘€π‘”Γ—π‘Ž+3𝑀𝑔×π‘₯ Rearranges to 𝑇= 5 6π‘Ž Γ— π‘€π‘”π‘Ž+3𝑀𝑔π‘₯ = 5𝑀𝑔 π‘Ž+3π‘₯ 6π‘Ž QED

19 2𝑀𝑔 =π‘‡π‘π‘œπ‘  ∝ WB 9b (exam Q cont )
The magnitude of the horizontal component of the force exerted on the plank at A by the wall is 2Mg Find x in terms of a b) Horizontally forces are in equilibrium 2𝑀𝑔 =π‘‡π‘π‘œπ‘  ∝ Mg 3Mg R=2Mg Friction a βˆ’π‘‡π‘π‘œπ‘  ∝ 𝑇 sin ∝ Substituting result from a) gives 2𝑀𝑔 = 5𝑀𝑔 π‘Ž+3π‘₯ 6π‘Ž π‘π‘œπ‘  ∝ 2𝑀𝑔 = 5𝑀𝑔 π‘Ž+3π‘₯ 6π‘Ž Γ— 4 5 Cancel by 2Mg to simplify gives 1 = π‘Ž+3π‘₯ 3π‘Ž Rearranges to a+3π‘₯ =3π‘Ž then to π‘₯= 2 3 π‘Ž

20 WB 9c (exam Q cont ) The force exerted on the plank at A by the wall acts in a direction which makes an angle Ξ² with the horizontal c) Find the value of tan 𝛽 c) Resolve forces vertically πΉπ‘Ÿπ‘–π‘π‘‘π‘–π‘œπ‘›+𝑇𝑠𝑖𝑛 ∝=4𝑀𝑔 Mg 3Mg R=2Mg Friction a βˆ’π‘‡π‘π‘œπ‘  ∝ 𝑇 sin ∝ πΉπ‘Ÿπ‘–π‘π‘‘π‘–π‘œπ‘›+ 5𝑀𝑔 π‘Ž+3π‘₯ 6π‘Ž Γ— 3 5 =4𝑀𝑔 Rearranges using π‘₯= 2 3 π‘Ž πΉπ‘Ÿπ‘–π‘π‘‘π‘–π‘œπ‘›=4π‘€π‘”βˆ’ 𝑀𝑔 π‘Ž+2π‘Ž 2π‘Ž = 5 2 Mg Now find tan  R=2Mg Friction = 5 2 Mg tan 𝛽 = 5 2 Mg 2𝑀𝑔 = 5 4 𝛽

21 simplify by cancelling and rearrange
WB 9d (exam Q cont ) The rope will break if the tension in it exceeds 5 Mg d) Explain how this will restrict the possible positions of P. You must justify your answer carefully previous results: 𝑇= 5𝑀𝑔 π‘Ž+3π‘₯ 6π‘Ž Mg 3Mg R=2Mg Friction= 2 5 𝑀𝑔 a βˆ’π‘‡π‘π‘œπ‘  ∝ 𝑇 sin ∝ we know: 𝑇= 5𝑀𝑔 π‘Ž+3π‘₯ 6π‘Ž ≀5𝑀𝑔 simplify by cancelling and rearrange 5 π‘Ž+3π‘₯ 6π‘Ž ≀5 5a+15x ≀30π‘Ž So the distance AP must be less than 5 3 π‘Ž For the rope NOT to break π‘₯ ≀ 5 3 π‘Ž

22 One thing to improve is –
KUS objectives BAT solve problems using moments and friction at angles to a rod/ object using sohCahToa self-assess One thing learned is – One thing to improve is –

23 END


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