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Chapter 11 : Kinematics of Particles

Engineering Dynamics. Chapter 11 : Kinematics of Particles. โดย สาขาวิชาวิศวกรรมเครื่องกล สำนักวิชาวิศวกรรมศาสตร์. Introduction. Mechanics ( กลศาสตร์ ) เป็นสาขาหนึ่งของวิทยาศาสตร์กายภาพที่ศึกษาและพิจารณาถึงสภาพของวัตถุเมื่อมีแรงกระทำเป็นผลให้วัตถุนั้น เคลื่อนที่ หรือ หยุดนิ่ง.

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Chapter 11 : Kinematics of Particles

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  1. Engineering Dynamics Chapter 11 : Kinematics of Particles โดย สาขาวิชาวิศวกรรมเครื่องกล สำนักวิชาวิศวกรรมศาสตร์

  2. Introduction Mechanics (กลศาสตร์) เป็นสาขาหนึ่งของวิทยาศาสตร์กายภาพที่ศึกษาและพิจารณาถึงสภาพของวัตถุเมื่อมีแรงกระทำเป็นผลให้วัตถุนั้น เคลื่อนที่ หรือ หยุดนิ่ง

  3. Introduction Mechanics แบ่งออกเป็น 2 ส่วน 1. Statics 2. Dynamics

  4. Introduction Statics (สถิตยศาสตร์) พิจารณาถึงการสมดุลของวัตถุที่อยู่กับที่ หรือ เคลื่อนที่ด้วยความเร็วคงที่ เมื่อมีแรงมากระทำ

  5. Introduction Dynamics (พลศาสตร์) พิจารณาถึงสภาพการเคลื่อนที่ของวัตถุภายใต้แรงกระทำ

  6. Introduction Dynamics แบ่งได้เป็น 2 ส่วน 1. Kinematics 2. Kinetics

  7. Introduction Kinematics(จลนคณิตศาสตร์) เป็นการศึกษาสภาพและเส้นทางการเคลื่อนที่ของวัตถุ โดยไม่พิจารณาถึงแรงที่กระทำต่อวัตถุ และสาเหตุที่ทำให้เกิดการเคลื่อนที่ กล่าวถึงความเชื่อมโยงกันของ ระยะทาง ความเร็ว และความเร่ง

  8. Introduction Kinetics(จลนศาสตร์) เป็นการศึกษาการเคลื่อนที่ของวัตถุ โดยพิจารณาถึงแรงที่กระทำต่อวัตถุนั้นด้วย กล่าวถึงความเชื่อมโยงกันของ แรง มวล และความเร่ง แรง การเคลื่อนที่ของวัตถุ

  9. Introduction ลักษณะของวัตถุที่สนใจ 1. Particle 2. Rigid Body

  10. Introduction Particle (อนุภาค) วัตถุใดๆ ที่มีมวล แต่จะไม่คำนึงถึงขนาดและรูปร่าง ทำให้เราจะพิจารณาวัตถุนั้นเป็นจุด หรือพิจารณาที่จุดศูนย์กลางมวลของวัตถุนั้น

  11. Introduction Rigid Body (วัตถุคงรูป) วัตถุใดๆ ที่มีมวล และคำนึงถึงขนาดและรูปร่าง ดังนั้นเมื่อมีการเคลื่อนที่ การวิเคราะห์ปัญหาจำเป็นต้องพิจารณาการหมุนรอบจุดศูนย์กลางมวลของวัตถุด้วย

  12. Motion of Particles Motion of Particles 1. Rectilinear Motion (การเคลื่อนที่เชิงเส้น) 2. Curvilinear Motion (การเคลื่อนที่ในแนวเส้นโค้ง)

  13. Rectilinear Motion of Particles Position Velocity Average velocity Instantaneous velocity

  14. Instantaneous acceleration Rectilinear Motion of Particles Acceleration Average acceleration

  15. Rectilinear Motion of Particles • Consider particle with motion given by • at t = 0, x = 0, v = 0, a = 12 m/s2 • at t = 2 s, x = 16 m, v = vmax = 12 m/s, a = 0 • at t = 4 s, x = xmax = 32 m, v = 0, a = -12 m/s2 • at t = 6 s, x = 0, v = -36 m/s, a = 24 m/s2

  16. Determination of the Motion of a Particles • Typically, conditions of motion are specified by the type of acceleration experienced by the particle. Determination of velocity and position requires two successive integrations. • Three classes of motion may be defined for: • acceleration given as a function of time, a = f(t) • - acceleration given as a function of position, a = f(x) • - acceleration given as a function of velocity, a = f(v)

  17. Acceleration given as a function of time, a = f(t): • Acceleration given as a function of position, a = f(x): Determination of the Motion of a Particles

  18. Determination of the Motion of a Particles • Acceleration given as a function of velocity, a = f(v):

  19. Sample 11.2 Ball tossed with 10 m/s vertical velocity from window 20 m above ground. • Determine: • velocity and elevation above ground at time t, • highest elevation reached by ball and corresponding time, and • time when ball will hit the ground and corresponding velocity.

  20. Sample 11.2 • SOLUTION: • Integrate twice to find v(t) and y(t).

  21. Solve for t at which velocity equals zero and evaluate corresponding altitude. Sample 11.2

  22. Sample 11.2 • Solve for t at which altitude equals zero and evaluate corresponding velocity.

  23. Sample 11.3 Brake mechanism used to reduce gun recoil consists of piston attached to barrel moving in fixed cylinder filled with oil. As barrel recoils with initial velocity v0, piston moves and oil is forced through orifices in piston, causing piston and cylinder to decelerate at rate proportional to their velocity; that is a = -kv Determine v(t), x(t), and v(x).

  24. SOLUTION: • Integrate a = dv/dt = -kv to find v(t). Sample 11.3 • Integrate v(t) = dx/dt to find x(t).

  25. Integrate a = v dv/dx = -kv to find v(x). • Alternatively, with and then Sample 11.3

  26. Uniform Rectilinear Motion For particle in uniform rectilinear motion, the acceleration is zero and the velocity is constant.

  27. Uniformly Accelerated Rectilinear Motion For particle in uniformly accelerated rectilinear motion, the acceleration of the particle is constant.

  28. relative position of B with respect to A relative velocity of B with respect to A relative acceleration of B with respect to A Motion of Several Particles: Relative Motion • For particles moving along the same line, time should be recorded from the same starting instant and displacements should be measured from the same origin in the same direction.

  29. Sample 11.4 Ball thrown vertically from 12 m level in elevator shaft with initial velocity of 18 m/s. At same instant, open-platform elevator passes 5 m level moving upward at 2 m/s. Determine (a) when and where ball hits elevator and (b) relative velocity of ball and elevator at contact.

  30. SOLUTION: • Substitute initial position and velocity and constant acceleration of ball into general equations for uniformly accelerated rectilinear motion. • Substitute initial position and constant velocity of elevator into equation for uniform rectilinear motion. Sample 11.4

  31. Write equation for relative position of ball with respect to elevator and solve for zero relative position, i.e., impact. • Substitute impact time into equations for position of elevator and relative velocity of ball with respect to elevator. Sample 11.4

  32. Position of block B depends on position of block A. Since rope is of constant length, it follows that sum of lengths of segments must be constant. constant (one degree of freedom) • Positions of three blocks are dependent. constant (two degrees of freedom) • For linearly related positions, similar relations hold between velocities and accelerations. Motion of Several Particles: Dependent Motion • Position of a particle may depend on position of one or more other particles.

  33. Sample 11.5 Pulley D is attached to a collar which is pulled down at 3 cm/s. At t = 0, collar A starts moving down from K with constant acceleration and zero initial velocity. Knowing that velocity of collar A is 12 cm/s as it passes L, determine the change in elevation, velocity, and acceleration of block B when block A is at L.

  34. Sample 11.5 • SOLUTION: • Define origin at upper horizontal surface with positive displacement downward. • Collar A has uniformly accelerated rectilinear motion. Solve for acceleration and time t to reach L.

  35. Sample 11.5 • Pulley D has uniform rectilinear motion. Calculate change of position at time t. • Block B motion is dependent on motions of collar A and pulley D. Write motion relationship and solve for change of block B position at time t.

  36. Sample 11.5 • Differentiate motion relation twice to develop equations for velocity and acceleration of block B.

  37. จบหัวข้อ 11.1-11.6

  38. Motion • 1. Rectilinear Motion • 2. Curvilinear Motion • - Rectilinear Components • - Tangential & Normal Components • - Radial & Transverse Components

  39. Consider particle which occupies position P defined by at time t and P’ defined by at t + Dt, instantaneous velocity (vector) instantaneous speed (scalar) Curvilinear Motion: Position, Velocity & Acceleration • Particle moving along a curve other than a straight line is in curvilinear motion. • Position vector of a particle at time t is defined by a vector between origin O of a fixed reference frame and the position occupied by particle.

  40. Consider velocity of particle at time t and velocity at t + Dt, instantaneous acceleration (vector) • In general, acceleration vector is not tangent to particle path and velocity vector. Curvilinear Motion: Position, Velocity & Acceleration

  41. Derivative of vector sum, • Derivative of product of scalar and vector functions, • Derivative of scalarproduct and vectorproduct, Derivatives of Vector Functions • Let be a vector function of scalar variable u, • Let be a scalar function of scalar variable u

  42. Velocity vector, • Acceleration vector, Rectangular Components of Velocity & Acceleration • When position vector of particle P is given by its rectangular components,

  43. Rectangular components particularly effective when component accelerations can be integrated independently, e.g., motion of a projectile, with initial conditions, Integrating twice yields • Motion of projectile could be replaced by two independent rectilinear motions. Rectangular Components of Velocity & Acceleration • Motion in horizontal direction is uniform. • Motion in vertical direction is uniformly accelerated.

  44. Position vectors for particles A and B with respect to the fixed frame of reference Oxyz are • Differentiating twice, • Vector joining A and B defines the position of B with respect to the moving frame Ax’y’z’ and velocity of B relative to A. acceleration of B relative to A. Motion Relative to a Frame in Translation • Designate one frame as the fixed frame of reference. All other frames not rigidly attached to the fixed reference frame are moving frames of reference. • Absolute motion of B can be obtained by combining motion of A with relative motion of B with respect to moving reference frame attached to A.

  45. are tangential unit vectors for the particle path at P and P’. When drawn with respect to the same origin, and is the angle between them. Tangential and Normal Components • Velocity vector of particle is tangent to path of particle. In general, acceleration vector is not. Wish to express acceleration vector in terms of tangential and normal components.

  46. With the velocity vector expressed asthe particle acceleration may be written as but After substituting, Tangential and Normal Components • Tangential component of acceleration reflects change of speed and normal component reflects change of direction. • Tangential component may be positive or negative. Normal component always points toward center of path curvature.

  47. Relations for tangential and normal acceleration also apply for particle moving along space curve. • Normal to the osculating plane is found from Tangential and Normal Components • Plane containing tangential and normal unit vectors is called the osculating plane. • Acceleration has no component along binormal.

  48. Similarly, the particle acceleration vector is Radial and Transverse Components • When particle position is given in polar coordinates, it is convenient to express velocity and acceleration with components parallel and perpendicular to OP. • The particle velocity vector is

  49. When particle position is given in cylindrical coordinates, it is convenient to express the velocity and acceleration vectors using the unit vectors • Position vector, • Velocity vector, • Acceleration vector, Radial and Transverse Components

  50. Sample 11.10 • SOLUTION: • Calculate tangential and normal components of acceleration. • Determine acceleration magnitude and direction with respect to tangent to curve. A motorist is traveling on curved section of highway at 88 m/s. The motorist applies brakes causing a constant deceleration rate. Knowing that after 8 s the speed has been reduced to 66 m/s, determine the acceleration of the automobile immediately after the brakes are applied.

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