Third Class Lever
 force is placed between the axis and resistance
 examples:
 tongs: food (R) is supported by grip on handles (F) while
axis is on opposite end.
 shovelling: dirt on shovel (R) is lifted by force to handle
by hand (F) while upper hand on end of shovel handle serves as
axis (A)
 rowing: oar is moved through water (R) by pulling on middle
of oar (F) while holding end of oar with opposite hand (A).
 Note: shovelling and rowing actions can also be first class
lever systems if the hand closes to the force remains stationary
(A) and the hand on the far end of the shovel or oar is moved
(F).
 batting: ball is hit (R) by moving bat toward ball with hand
of far arm (F) while supporting lower portion of bat with hand
of near arm (A).
 example in body
 most levers in body are third class
 elbow flexion
 Biceps and brachialis pull ulna (F)
lifting the forearm, hand, and any load (R) at the elbow (A).
 knee flexion
 hamstring contract (F) to flex the lower leg (R) at the knee
(A).
 lever characteristics
 produces speed and range of motion
 requires relatively great force to move even small resistances
 weight machines: less resistance required, greater inertia
 harder to start and stop movement
Lever Arm Length
 Definitions
 Resistance Arm: distance between axis and point of resistance
application.
 Force Arm: distance between axis and point of force.
 Formula
F 
x 
FA 
= 
R 
x 
RA 
Force 
x 
Force Arm 
= 
Resistance 
x 
Resistance Arm 
Initial Example 

Change insertion 1 cm 

Change point of resistance 1 cm 
F x 2 cm 
= 
10 kg x 9 cm 
2 F 
= 
90 kg 
F 
= 
45 kg 


F x 3 cm 
= 
10 kg x 9 cm 
3 F 
= 
90 kg 
F 
= 
30 kg 


F x 2 cm 
= 
10 kg x 8 cm 
2 F 
= 
80 kg 
F 
= 
40 kg 

 Lever characteristics
 Long resistance arm: speed and range of movement
 Short resistance arm: force
 Mechanical advantage
 Motive force arm length / Resistive force arm length
 No mechanical advantage if quotient = 1 (same length):
 If quotient >1: mechanical advantage in force
 If quotient <1: mechanical advantage in speed and range
of motion
 Lever length of resistive forces
 Center of gravity of body segment (eg: forearm in arm curl,
body during pushup, etc.)
 Center of gravity of any additional weight. (eg: handle on
barbell, sand bag on back, etc.)
 Perpendicular distance from fulcrum
 When calculating forces applied to levers, the Perpendicular
Distance from the fulcrum needs to be measured.
 Torque = Force x Perpendicular Distance.
 The physical distance and the perpendicular distance are
the same only when force is being applied at a right angle (perpendicular)
to the lever.
 Perpendicular distance can be calculated by multiplying the
physical distance x sine of the angle of force application. Also
see Force Vectors and example below.
Variable Resistance Levers

Resistive force (R) is initially relatively short [close to fulcrum
(A)]. 


As motive force (F) acts on lever, resistive arm becomes physically
longer yet its perpendicular distance remains constant. In contrast,
motive torque deminishes requiring progressively greater motive
force throughout movement. 

Even though the physical distance between the (R) resistive force
and (A) fulcrum increases approximately 2 fold, perpendicular
distance is the same. You can more clearly see this by drawing
a line in the direction of (R) resistive force and a parallel
line through (A) fulcrum. Since gravity acts on the weight in
our diagram, the (R) restive force is downward, so both lines
will be drawn vertically. The distance between the lines (perpendicular
distance) are the same in each diagram, therefore the resistive
torque remains constant.
In contrast, although the physical distance between the (F)
motive force and (A) fulcrum do not change, their perpendicular
distance decrease. To see this, draw a line in the direction
of the (F) motive force and a parallel line through the (A) fulcrum.
But in this case the distance between the lines (perpendicular
distance) decrease, therefore the motive torque diminishes as
it moved downward, requiring greater (F) motive forces to raise
the (R) resistive forces.

