🏎️Engineering Mechanics – Dynamics Unit 2 – Kinetics of Particles in Engineering Mechanics
Kinetics of Particles in Engineering Mechanics builds on kinematics, focusing on forces and their effects on motion. It covers Newton's laws, work, energy, power, impulse, and momentum, providing tools to analyze and predict particle behavior under various forces.
This unit connects fundamental physics principles to real-world engineering applications. Students learn to solve complex problems involving particle dynamics, energy transfer, and collisions, developing critical skills for designing and analyzing mechanical systems.
Particle a body with a mass but negligible size and shape, treated as a point
Kinematics the study of motion without considering the forces causing it, focusing on position, velocity, and acceleration
Dynamics the study of forces and their effects on motion, building upon kinematics
Inertia the resistance of an object to changes in its motion, related to its mass
Force a push or pull acting on an object, causing it to accelerate if unbalanced
Contact forces (friction, normal force) result from direct contact between objects
Action-at-a-distance forces (gravity, electromagnetism) act without direct contact
Momentum the product of an object's mass and velocity, a vector quantity
Work the product of force and displacement, a scalar quantity measuring energy transfer
Energy the capacity to do work, existing in various forms (kinetic, potential, thermal)
Kinetic energy 21mv2, energy of motion
Potential energy energy due to position or configuration (gravitational, elastic)
Kinematics of Particles
Position the location of a particle in space, typically described using Cartesian coordinates (x,y,z)
Displacement the change in position of a particle, a vector quantity
Velocity the rate of change of position with respect to time, the first derivative of position v=dtdr
Average velocity vavg=ΔtΔr, the displacement divided by the time interval
Instantaneous velocity v=limΔt→0ΔtΔr, the velocity at a specific instant in time
Acceleration the rate of change of velocity with respect to time, the second derivative of position a=dtdv
Average acceleration aavg=ΔtΔv, the change in velocity divided by the time interval
Instantaneous acceleration a=limΔt→0ΔtΔv, the acceleration at a specific instant in time
Kinematic equations a set of equations describing the motion of a particle under constant acceleration
v=v0+at
r=r0+v0t+21at2
v2=v02+2a⋅(r−r0)
Newton's Laws and Particle Dynamics
Newton's first law an object at rest stays at rest, and an object in motion stays in motion with constant velocity, unless acted upon by an unbalanced force
Newton's second law the acceleration of an object is directly proportional to the net force acting on it and inversely proportional to its mass F=ma
Newton's third law for every action (force), there is an equal and opposite reaction (force)
Free body diagram a graphical representation of all the forces acting on an object, used to analyze the net force
Friction a force that opposes the relative motion between two surfaces in contact
Static friction fs≤μsN, the force preventing an object from starting to move
Kinetic friction fk=μkN, the force opposing the motion of an object sliding on a surface
Tension the force transmitted through a rope, string, or cable pulling on an object
Normal force the force exerted by a surface on an object in contact with it, perpendicular to the surface
Work, Energy, and Power
Work the product of force and displacement in the direction of the force W=F⋅d
Positive work done by a force in the same direction as the displacement
Negative work done by a force opposite to the direction of displacement
Work-energy theorem the net work done on an object equals the change in its kinetic energy Wnet=ΔKE
Conservative force a force for which the work done is independent of the path taken (gravity, spring force)
Potential energy associated with conservative forces, ΔPE=−Wcons
Non-conservative force a force for which the work done depends on the path taken (friction, air resistance)
Conservation of energy the total energy of a closed system remains constant, energy cannot be created or destroyed, only converted between forms
Power the rate at which work is done or energy is transferred P=dtdW=F⋅v
Average power Pavg=ΔtW, the total work divided by the time interval
Instantaneous power P=limΔt→0ΔtΔW, the power at a specific instant in time
Impulse and Momentum
Impulse the product of force and time, equal to the change in momentum J=FΔt=Δp
Conservation of momentum the total momentum of a closed system remains constant, momentum is neither created nor destroyed, only transferred between objects
Elastic collision a collision in which both momentum and kinetic energy are conserved
Inelastic collision a collision in which momentum is conserved but kinetic energy is not, some energy is converted to other forms (heat, deformation)
Coefficient of restitution a measure of the elasticity of a collision, the ratio of the final to initial relative velocities e=−v2i−v1iv2f−v1f
Perfectly elastic collision e=1, kinetic energy is conserved
Perfectly inelastic collision e=0, objects stick together after the collision
Center of mass the point at which the entire mass of a system can be considered to be concentrated rcm=∑mi∑miri
Rocket equation describes the motion of a rocket, based on the conservation of momentum Δv=velnmfm0
Relative Motion and Moving Reference Frames
Relative position the position of one object with respect to another, rA/B=rA−rB
Relative velocity the velocity of one object with respect to another, vA/B=vA−vB
Relative acceleration the acceleration of one object with respect to another, aA/B=aA−aB
Galilean transformation equations relating position, velocity, and acceleration between two reference frames moving with constant relative velocity
r′=r−vframet
v′=v−vframe
a′=a
Coriolis acceleration an apparent acceleration experienced by an object moving in a rotating reference frame acor=−2ω×v′
Centrifugal acceleration an apparent acceleration directed away from the axis of rotation in a rotating reference frame acf=−ω×(ω×r′)
Applications and Problem-Solving Strategies
Identify the system and draw a free body diagram showing all the forces acting on the object(s) of interest
Determine the known and unknown quantities, and choose appropriate coordinate axes
Apply Newton's second law F=ma to relate the forces to the acceleration
Use kinematic equations to relate position, velocity, and acceleration
Apply the work-energy theorem Wnet=ΔKE or conservation of energy to solve for unknown quantities
Apply the impulse-momentum theorem J=Δp or conservation of momentum to solve for unknown quantities
For relative motion problems, choose appropriate reference frames and apply Galilean transformations or consider Coriolis and centrifugal accelerations if necessary
Check the units and reasonableness of the answer, and consider any limiting cases or special conditions
Advanced Topics and Extensions
Angular kinematics and dynamics extending the concepts of linear motion to rotational motion, considering angular position, velocity, acceleration, and torque
Rigid body dynamics analyzing the motion of extended objects, considering both translation and rotation
Lagrangian mechanics an alternative formulation of mechanics based on the principle of least action, using generalized coordinates and energies
Hamiltonian mechanics a reformulation of Lagrangian mechanics using generalized momenta and Hamilton's equations
Variational principles the principle of least action and Hamilton's principle, which state that the path followed by a system minimizes a certain functional (action)
Noninertial reference frames reference frames that are accelerating or rotating, requiring the inclusion of fictitious forces (Coriolis, centrifugal)
Relativistic mechanics the extension of Newtonian mechanics to high-speed motion, considering the effects of special relativity (time dilation, length contraction, mass-energy equivalence)
Continuum mechanics the study of the mechanics of continuous media, such as fluids and deformable solids, using concepts like stress, strain, and constitutive relations