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Physics 13 General Physics 1

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1 Physics 13 General Physics 1
Dynamics of Motion: Application of Newtonโ€™s Laws of Motion MARLON FLORES SACEDON

2 Application of Newtonโ€™s Laws of Motion
Friction Friction ๐‘“ - refers to actual forces that are exerted to oppose motion - a resistance that opposes every effort to slide or roll a body over another Kinds of Friction: 1. Static friction - force that will just start the body. 2. Kinetic friction - force that will pull the body uniformly. Coefficient of friction ๐œ‡ - the ratio of the force necessary to move one surface over the other with uniform velocity to the normal force pressing the two surfaces to other. ๐œ‡= ๐‘“ ๐‘ ๐‘“=๐œ‡๐‘ Where: N is the normal force exerted by the contact surface to the object. ๐‘ฆ ๐‘ฅ ๐‘ฆ ๐‘ฅ ๐‘ฆ ๐‘ฅ ๐‘ ๐‘ ๐‘ ๐‘ƒ ๐‘“ ๐‘ƒ m m ๐‘“ m ๐‘“ ๐‘ค ๐‘ค ๐œƒ ๐œƒ ๐‘ค

3 Application of Newtonโ€™s Laws of Motion
Free-Body Diagram (FBD) FBD is a vectors diagram showing all forces acting on the body. ๐‘ฆ ๐‘ฅ m ๐‘ ๐‘ƒ ๐‘ค ๐‘“ ๐œƒ

4 Application of Newtonโ€™s Laws of Motion
Free-Body Diagram (FBD) FBD is a vectors diagram showing all forces acting on the body. ฮฃ ๐น ๐‘ฆ =๐‘โˆ’๐‘ค=0 (for static equilibrium) ๐‘ฆ ๐‘ฅ ๐œฎ ๐‘ญ ฮฃ ๐น ๐‘ฅ =๐‘ƒโˆ’๐‘“ (Net External force) ๐’‚ N FBD of Furniture ๐œฎ ๐‘ญ = ๐‘ƒ ๐‘ฅ โˆ’๐‘“ Net external force ๐’‡=๐๐‘ต Note: If pulling force ๐‘ƒ is less than friction ๐‘“ then furniture is at rest otherwise it will move to the right.. ๐‘ท ๐’˜=๐’Ž๐’ˆ

5 Application of Newtonโ€™s Laws of Motion
Free-Body Diagram (FBD) FBD is a vectors diagram showing all forces acting on the body. FBD of box ๐‘ฆ ๐‘ฅ ๐œฎ ๐‘ญ ฮฃ ๐น ๐‘ฆ =๐‘+ ๐‘ƒ ๐‘ฆ โˆ’๐‘ค=0 (for static equilibrium) N ๐’‚ ฮฃ ๐น ๐‘ฅ = ๐‘ƒ ๐‘ฅ โˆ’๐‘“ (Net External force) P ๐‘ท ๐’š ๐œฎ ๐‘ญ = ๐‘ƒ ๐‘ฅ โˆ’๐‘“ ๐’‡=๐๐‘ต Net external force ๐’˜=๐’Ž๐’ˆ ๐‘ท ๐’™ Note: If ฮฃ ๐น ๐‘ฆ is not equal to zero then box didnโ€™t touch the ground surface. Therefore Net external force is not equal to ฮฃ ๐น ๐‘ฅ .

6 Application of Newtonโ€™s Laws of Motion
Free-Body Diagram (FBD) Exercise Problem: Construct the free-body diagram (FBD) FBD of box ๐œฎ ๐‘ญ ๐’‚ ๐‘ฆ ๐‘ฅ N ๐’‡=๐๐‘ต ๐’˜=๐’Ž๐’ˆ ๐’˜ ๐’™ ๐’˜ ๐’š 20 ๐‘œ

7 Application of Newtonโ€™s Laws of Motion
Problem: A horizontal cord is attached to a 6.0-kg body in a horizontal table. The cord passes over a pulley at the end of the table and to this end is hung a body of mass 8 kg. Find the distance the two bodies will travel after 2s, if they start from rest. What is the tension in the cord? ๐‘  ๐‘ก=2๐‘  Figure: ๐‘š ๐ด ๐‘š ๐ต ๐‘š ๐ด ๐‘š ๐ต ๐‘š ๐ต ๐‘š ๐ด ๐‘  ๐‘ก=2๐‘ 

8 Application of Newtonโ€™s Laws of Motion
Problem: A horizontal cord is attached to a 6.0-kg body in a horizontal table. The cord passes over a pulley at the end of the table and to this end is hung a body of mass 8 kg. Find the distance the two bodies will travel after 2s, if they start from rest. What is the tension in the cord? ๐‘ฆ ๐‘ฅ ฮฃ ๐น ๐ด ๐‘ โˆ’๐‘‡ ๐‘๐‘œ๐‘Ÿ๐‘‘ ๐‘ฆ ๐‘ฅ FBD of ๐‘š ๐ด FBD of ๐‘š ๐ต ๐‘Ž ๐‘ฆ ๐‘ฅ ๐‘  ๐‘ก=2๐‘  Figure: +๐‘‡ ๐‘๐‘œ๐‘Ÿ๐‘‘ ฮฃ ๐น ๐ต ๐‘Ž ๐‘š ๐ด ๐‘š ๐ต ๐‘š ๐ด ๐‘š ๐ต ๐‘š ๐ด ๐‘š ๐ต ๐‘š ๐ต ๐‘š ๐ด โˆ’๐‘ค ๐ด = ๐‘š ๐ด ๐‘” ๐‘ค ๐ต = ๐‘š ๐ต ๐‘” ๐‘ฆ ๐‘ฅ ฮฃ ๐น ๐‘ฆ =๐‘โˆ’ ๐‘ค ๐ด =0 (static equilibrium) ๐‘  ๐‘ก=2๐‘  ฮฃ ๐น ๐‘ฅ = +๐‘‡ ๐‘๐‘œ๐‘Ÿ๐‘‘ ฮฃ ๐น ๐‘ฆ =0 (static equilibrium) Net external force ฮฃ ๐น ๐‘ฅ = โˆ’๐‘‡ ๐‘๐‘œ๐‘Ÿ๐‘‘ + ๐‘š ๐ต ๐‘” Net external force ฮฃ ๐น ๐ด = ๐‘š ๐ด ๐‘Ž From Second law ฮฃ ๐น ๐ต = ๐‘š ๐ต ๐‘Ž From Second law Add ๐ธ๐‘ž 1and ๐ธ๐‘ž.2 to eliminate ๐‘‡ ๐‘๐‘œ๐‘Ÿ๐‘‘ then solve Acceleration ๐‘Ž. ๐‘‡ ๐‘๐‘œ๐‘Ÿ๐‘‘ = ๐‘š ๐ด ๐‘Ž Eq.1 โˆ’๐‘‡ ๐‘๐‘œ๐‘Ÿ๐‘‘ + ๐‘š ๐ต ๐‘”= ๐‘š ๐ต ๐‘Ž Eq.2 ๐‘Ž= ๐‘š ๐ต ๐‘” ๐‘š ๐ด + ๐‘š ๐ต ๐‘Ž= 8(9.81) 6+8 =5.61๐‘š/ ๐‘  2 Contโ€™n

9 Application of Newtonโ€™s Laws of Motion
Problem: A horizontal cord is attached to a 6.0-kg body in a horizontal table. The cord passes over a pulley at the end of the table and to this end is hung a body of mass 8 kg. What is the tension in the cord? Find the distance the two bodies will travel after 2s, if they start from rest. ๐‘ฆ ๐‘ฅ a) Solve for tension in the cord ๐‘‡ ๐‘๐‘œ๐‘Ÿ๐‘‘ using Eq.1 ๐‘  ๐‘ก=2๐‘  Figure: ๐‘‡ ๐‘๐‘œ๐‘Ÿ๐‘‘ =6(5.61)=33.66 N ANSWER ๐‘š ๐ด ๐‘š ๐ต ๐‘š ๐ด ๐‘š ๐ต ๐‘š ๐ต ๐‘š ๐ด ๐‘ฆ ๐‘ฅ b) Solve for the distance ๐‘  of two bodies after travelling 2 sec. Given: ๐‘  ๐‘ก=2๐‘  ๐‘ฃ ๐‘– =0 ๐‘ก=2 ๐‘  ๐‘Ž=5.61 ๐‘š/ ๐‘  2 From kinematics: ๐‘ = ๐‘ฃ 1 ๐‘ก ๐‘Ž ๐‘ก 2 ๐‘ = =11.22๐‘š ANSWER

10 ASSIGNMENT Figure: . Given: m = 10 kg h = 5 m L = 10m S1 = 2m ร˜ =44o
๐œ‡=0.06 coef. of kinetic friction Note: Particle โ€œmโ€ is release from rest at pt. A and moves to pt. B, then to pt.C, and finally to pt.D. Neglect the effect of the change in velocity direction at pt.B. The same value of coef. friction, from pt.A to pt.C. Projectile motion from pt.C to pt.D. Required: a. Free-body diagram of the particle at inclined plane AB. b. Free-body diagram of the particle at horizontal plane BC. c. Unbalanced force of the particle along the inclined plane AB. d. Unbalanced force of the particle along the horizontal plane BC. e. acceleration, a1 of the particle along the inclined plane AB. f. acceleration, a2 of the particle along the horizontal plane BC. g. velocity of the particle at pt.B. h. velocity of the particle at pt.C. i. Range, (S2) j. Total time of travel of particle from pt A to pt. D. ASSIGNMENT Figure:

11 ASSIGNMENT

12 ASSIGNMENT

13 ASSIGNMENT

14 eNd


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