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Transcript
Torque
•
Torque
Torque, τ, is the tendency of a force to rotate
an object about some axis
•
•
Lever arm (d1, d2) is the
perpendicular line
connecting the point of
rotation to the line-ofaction of the applied force.
By convention, torques
that produce
•
Torque is a vector
τ = r F sin φ = F d
•
•
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F is the force
φ is the angle the force makes with the horizontal
d is the moment arm (or lever arm)
•
•
Torque
•
Which force
produces the most
torque?
counterclockwise rotation
are positive.
clockwise rotation are
negative.
Torque, cont
•
The moment arm, d, is the
perpendicular distance from
the axis of rotation to a line
drawn along the direction of
the force
•
•
d = r sin φ
Alternatively, take
perpendicular component of
force.
1
Torque, final
•
•
The horizontal component of F (F cos φ) has
no tendency to produce a rotation
Torque will have direction
•
•
•
•
•
•
The force F1 will tend to
cause a counterclockwise
rotation about O
The force F2 will tend to
cause a clockwise rotation
about O
Στ = τ1 + τ2 = F1d1 – F2d2
Torque vs. Force
Torque Units
Forces can cause a change in linear
motion
•
•
•
If the turning tendency of the force is
counterclockwise, the torque will be positive
If the turning tendency is clockwise, the torque will
be negative
Net Torque
•
•
Described by Newton’s Second Law
Forces can cause a change in rotational
motion
•
The SI units of torque are N.m
The effectiveness of this change depends
on the force and the moment arm
The change in rotational motion depends
on the torque
•
Although torque is a force multiplied by a
distance, it is very different from work and
energy
The units for torque are reported in N.m
and not changed to Joules
2
Torque and Angular Acceleration,
Wheel Example
Torque and Angular Acceleration
•
•
τ = Iα
The torque is directly proportional to the
angular acceleration and the constant of
proportionality is the moment of inertia
Energy in an Atwood Machine,
Example
•
•
•
•
The wheel is rotating and
so we apply Στ = Ια
• The tension supplies the
tangential force
The mass is moving in a
straight line, so apply
Newton’s Second Law
• ΣF y = may = mg - T
Summary of Useful Equations
The blocks undergo
changes in
translational kinetic
energy and
gravitational
potential energy
The pulley
undergoes a change
in rotational kinetic
energy
3