1/35
Looks like no tags are added yet.
Name | Mastery | Learn | Test | Matching | Spaced |
|---|
No study sessions yet.
Energy of motion
translational kinetic energy
K = ½ * mv²
depends of reference frame (observer’s view)
Hooke’s Law
Fs = -k * delta x
If there is friction, the work done by friction reduces the kinetic energy:
If there is friction, the work done by friction reduces the kinetic energy:
Kfinal=Kinitial+Wspring+WfrictionKfinal=Kinitial+Wspring+Wfriction
Work
amount of mechanical energy transferred into or out of system
Constant force = W = Fdcostheta
Theta = angle between direction of F and d
Work done by a conservative force in system
independent of path of object
Depends on initial and final configurations
If displacement 0, zero work done and change in potential energy is zero.
Nonconservative force examples
force of friction and force of air resistance (also called drag force)
Work done by a nonconservative force
Does depend on the path
Displacement under Fcostheta vs. x graph
equals work
3 types of mechanical energy
kinetic energy
Gravitational potential energy
Elastic potential energy
Potential energy
energy stored in a system due to positions of objects in system
Gravitational potential energy in constant gravitational field equation
Pg = mgh
change in gravitational potential energy in constant gravitational field
Delta Ug = mg * delta y
Vertical height above horizontal zero line
h or y
Symbols for potential energy
PE and U
Potential signs of PE and KE
PE can be negative (b/c h can be negative)
KE can’t be negative
Ug between two objects w mass
- (Gm1m2)/r
G is gravitational constant
R is distance between centers of mass of the two objects
Ug = 0
where both objects are infinitely far away from one another (r = infinity)
Why general form of Ug is always negative
Gravitational constant
G = 6.67 × 10^-11 (N*m²)/kg²
Elastic potential energy
PEe = Ue = ½ k(delta x)²
energy stored in a mass-spring system
Ue can’t be negative
Mechanical energy of a system
some of systems K, PEg, and PEe
System w one object
can only have kinetic energy
Conservation of energy
any changes to the types of energies in a system are balanced by equivalent changes of other types of energies in the system or by a transfer of energy into or out of the system.
When total mechanical energy remains same
ME = ME
zero net work done on system and zero work done by nonconservative forces
Work-Energy Principle
net work equals change in kinetic energy principle
Wnet = delta K
Can be used when work is done by nonconservative forces on system
Power
rate at which energy changes with respect to time, by either being transferred into or out of the system or converted from one type of energy to another within a system
Rate at which wrk is done on a system
Average power formula
Pavg = delta E/delta t = W/delta t
Instantaneous Power
Fvcostheta
v is instantaneous velocity of system or object
F parallel
Fcostheta
Power units
Watts, (kg * m²)/s³
Examples of conservative force
gravity force, spring force
Energy definition
ability to do work (scalar) in joules
Internal energy
heat energy that causes an increase in the temp of te system
Work done by friction
Ffriction*d*costheta
Work energy Principle
Ui + Ki + Wnc = Uf + Kf
Work energy theorem
net work done on an object is equal to its change in kinetic energy
Wnet = delta K = KEf - KEi
Wnet = ½ *mvf² - ½ *mvi²
In system with no earth
There is no potential energy, just kinetic