1/15
Fill-in-the-blank practice flashcards derived from lecture notes covering work, energy, work-energy theorem, power, potential energy types, and conservative vs non-conservative forces.
Name | Mastery | Learn | Test | Matching | Spaced | Call with Kai | Chat |
|---|
No analytics yet
Send a link to your students to track their progress
Work is said to be done by an applied force when it produces __________.
displacement
The small amount of work done dW by a force F for a small displacement dr is given by dW=F⋅dr, and its unit is the __________.
Joule
The Work-Energy Theorem states that work done is equal to the change in __________.
kinetic energy
Using the kinematic relation v2=u2+2aS, the work done W=FS=maS simplifies to W= __________.
21mv2−21mu2
The formula relating kinetic energy (K.E.) and linear momentum (p) for a body of mass m is K.E.= __________.
2mp2
Linear momentum p expressed in terms of mass m and kinetic energy (K.E.) is p= __________.
2m(K.E.)
Power is defined as the rate of work done or __________ delivered.
energy
One horsepower (1hp) is equal to __________.
746W
The expression for power P in terms of force F and velocity v is P= __________.
F⋅v
The formula for gravitational potential energy U with mass m, acceleration due to gravity g, and height h is U= __________.
mgh
The elastic potential energy U stored in a spring with spring constant k and displacement x is U= __________.
21kx2
For a conservative force, the work done is __________ of the path.
independent
The total work done by a conservative force in a round trip is __________.
zero
Examples of conservative forces mentioned in the notes include gravitational force, elastic force, and __________ force.
Magnetic
For a non-conservative force, energy is dissipated as __________ on the surface.
heat
Two examples of non-conservative forces are frictional force and __________ force.
viscous