Physics Exam 2

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81 Terms

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kinetic energy equation

½ mv2

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work energy principle

change in kinetic energy

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total mechanical energy =

KE + PE

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mechanical energy stays constant as long as no

nonconservative forces do work

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radial (centripetal) acceleration

aR = v2/r

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where is acceleration directed at in uniform circular motion

center of the circle

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frequency

number of revolutions per second

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period

time required fro one complete revolution

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period equation

1/f

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net force equation for UCM

m v2/r

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conservative forces

do not change direction of work

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nonconservative forces

do change/depend on direction of work

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apparent weight

the force an object appears to exert on a scale/surface

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gravitational potential energy equation

PEG=mgy

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elastic potential energy

PE= ½ kx2

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law of conservation of energy

total energy can be transformed and transferred but total amount remains constant in system

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dissipative forces

reduce mech. energy, but not total energy, due to friction

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work done by nonconservative forces

WNC= -FFrd

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Power

rate at which work is done

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power equation

P= W/t

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power in terms of net force applied

P= Fv

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linear momentum equation

p=mv

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newton’s second law in terms of momentum

F= m v/t

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if no external forces act on a system,

the momentum is a conserved quantity

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the more momentum an object has,

the harder is it to stop it

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impulse equation

F (t) = change in p

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elastic collision

two hard objects collide and no energy is produced in collision; total KE is same before and after

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if KE is conserved during a collision then,

it is an elastic collision

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if KE is not conserved during a collision then,

it is an inelastic collision

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objects in elastic collisions bounce away

at same speed as beginning

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objects in inelastic collisions bounce away

at lesser speed than initially

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if two objects stick together after a collision,

the collision is completely in inelastic

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axis of rotation

all points on a object moving in rotational motion and the center circle lie here

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angular position

how far a rotating object has rotated

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how to find angular position

specify angle of particular line in object measured along circumference of path

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radian

use length distance from axis to calculate

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radian equation

θ=arclength⁡r\theta=\frac{arcleng\operatorname{th}}{r}

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angular velocity and angular acceleration

are the same at every point in RM

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angular displacement

measures how far an object rotates

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average angular velocity equation

ω=ΔθΔt\omega=\frac{\Delta\theta}{\Delta t}

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instantaneous angular velocity

limit of average angular velocity as t approaches 0

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angular velocity units

rad/s

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angular acceleration

change in angular velocity over change in time

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angular acceleration symbol

α\alpha

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do rotating objects with angular velocities have linear velocities

yes, direction is tangent to its circular path

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linear velocity equation for RM

v=rωv=r\omega

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an object’s linear velocity is _____ for points farther from axis

greater

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tangential acceleration of a point on a rotating object

atan⁡=rαa\tan=r\alpha

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the total linear acceleration of a point in rotation is the vector sum of

tangential acceleration and centripetal acceleration

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centripetal acceleration equation

aR=ω2raR=\omega^2r

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aRaR is ____ the farther from the center

greater

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frequency

number of completed revolutions per second

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frequency (f) is related to angular velocity by

ω=2πf\omega=2\pi f

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frequency unit

Hertz

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period

time required for one complete revolution

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period equation

1f\frac{1}{f}

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rolling objects without slipping requires both

translational and rotational motion

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lever arm

distance from axis of rotation of a rotating object

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angular acceleration is proportional to

torque

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torque symbol

τ\tau

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the smaller the lever arm,

the least effective in accelerating the object

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torque units

m N

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which forces only cause rotational acceleration

forces perpendicular to axis of rotation

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torque equation

τ=Iα\tau=I\alpha

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rotational inertia symbol

II

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rotational inertia equation

mr2mr^2

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fixed rotational KE equation

12Iω2\frac12I\omega^2

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moving rotational KE equation

12mv2+12Iω2\frac12mv^2+\frac12I\omega^2

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static friction must be present for

an object to roll

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does static friction do any work on a rolling object

no, too small to measure

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what causes rolling objects to slow down

some gravitational potential energy is converted to rotational KE, leaving less for translational KE

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work done by torque equation

W=τΔθW=\tau\Delta\theta

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power from applied torque

p=τωp=\tau\omega

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angular momentum equation

L=IωL=I\omega

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units for angular momentum

kg⁡⋅m2s\operatorname{kg}\cdot\frac{m^2}{s}

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Newton’s 2nd law of rotation in terms of angular momentum

τ=ΔLΔt\tau=\frac{\Delta L}{\Delta t}

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Law of Conservation of Angular Momentum

the total angular momentum of a rotating object remains constant if the net torque acting on it is zero

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center of mass

the point in an object or a system of objects that moves in the same path that a particle would move if subjected to the same force

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center of mass of a system equation

xcm⁡=(maxa+mbxb+mcxc)Mx_{\operatorname{cm}}=\frac{\left(m_{a}x_{a}+m_{b}x_{b}+m_{c}x_{c}\right)}{M}

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if one mass in a system is greater than the other, then the CM is

closer to the larger mass

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center of gravity is considered to be

the same as center of mass