theTreeSpyder
TreeHouser
- Joined
- Feb 12, 2016
- Messages
- 691
Most leverage we think of is by right angle, involves length.
flexible levers/ropes do not resist on the cross axis,therefore there is no length multiplier
>>leverage is by stacked sequential 1x pulls additively, not multiplying geometrically like rigid lever
.
Pulleys pull inline, not at right angle.
>>Pulleys simply add another inline pull against the load @ given rope tension(ignoring frictions)
>>can view as making lever longer in some ways, in 1 unit even increments (right angle lever can get 5.34 leverage etc.)
.
For simple systems : adding 1x increment legs of pull via pulley
A typical line of force has the pull equal and opposite on both ends;
a pulley system can simply take flexible line, and fold back the running away; equal/opposite direction force
>>and fold it back/recycle force to work on the load again.
Only moving pulleys allow another sequential leg of pull on load
>>fixed/anchored pulleys just are redirects/re-positioning forces/directions
>>note just as can multiply force on load, can do same on anchor(s), system can reverse, if anchor moves it becomes load in scenario
.
for compound systems that each have anchor out of the system:
the output of the systems are multiplied, a 3:1 into a 5:1 =15:1
BUT each pulley has frictions, and the inefficiencies of the chain of inefficiencies would be a multiplying tax against the output.
.
for compound systems that 1 system has no anchor :
the output the system w/o anchor pulls 2 multiplying paths into the next system
kinda my 2handing example set to pulleys.
.
Back to simplest system imagery:
BUT , this all assUme's each leg of line is pulled PURE INLINE to get the maximum potential pull of 1x per leg on load.
The more angle of deflection from PURE INLINE, the less the return on the pull, between 0-1 range multiplier is used to calculate.
>>This 0-1 range multiplier for potential (the total pull) gives the amount of pull actually working on load (ignoring frictions)
We call this 0-1 range multiplier :COSINE(cos).
.
Cosine of 30 is .8666 so if pulling 100# tension, only realize 86.66 on pulley
>>and 50# pulling across cuz SINE(sin) is. 5. ( i think riggers and climbers should be familiar with benchmark sine/cosines of 0,15,30,45,90)
So can say, each leg of load pull adds it's cosine x rope tension as a pull against load .
>>we assUme each leg is 0degrees deflection and that that cosine is the 1.0 we assUme
note:on spread to 2 points, only look at half the spread as the angle of deflection for each pull/support
.
Once grasp that, same math for hanging picture with 2 spread anchors on picture and 1 nail in wall
>>the tension on wire is raised so has enough inline force /cosine to pull up on picture
>>incurring the sine as tax for business at that angle
>>this tax can sidewards pull anchors off picture from sine forces produced.
.
my mnemonic:
so politically speaking: Don't let your SIN corrupt your COS(cause)!
.
time to clock in!
flexible levers/ropes do not resist on the cross axis,therefore there is no length multiplier
>>leverage is by stacked sequential 1x pulls additively, not multiplying geometrically like rigid lever
.
Pulleys pull inline, not at right angle.
>>Pulleys simply add another inline pull against the load @ given rope tension(ignoring frictions)
>>can view as making lever longer in some ways, in 1 unit even increments (right angle lever can get 5.34 leverage etc.)
.
For simple systems : adding 1x increment legs of pull via pulley
A typical line of force has the pull equal and opposite on both ends;
a pulley system can simply take flexible line, and fold back the running away; equal/opposite direction force
>>and fold it back/recycle force to work on the load again.
Only moving pulleys allow another sequential leg of pull on load
>>fixed/anchored pulleys just are redirects/re-positioning forces/directions
>>note just as can multiply force on load, can do same on anchor(s), system can reverse, if anchor moves it becomes load in scenario
.
for compound systems that each have anchor out of the system:
the output of the systems are multiplied, a 3:1 into a 5:1 =15:1
BUT each pulley has frictions, and the inefficiencies of the chain of inefficiencies would be a multiplying tax against the output.
.
for compound systems that 1 system has no anchor :
the output the system w/o anchor pulls 2 multiplying paths into the next system
kinda my 2handing example set to pulleys.
.
Back to simplest system imagery:
BUT , this all assUme's each leg of line is pulled PURE INLINE to get the maximum potential pull of 1x per leg on load.
The more angle of deflection from PURE INLINE, the less the return on the pull, between 0-1 range multiplier is used to calculate.
>>This 0-1 range multiplier for potential (the total pull) gives the amount of pull actually working on load (ignoring frictions)
We call this 0-1 range multiplier :COSINE(cos).
.
Cosine of 30 is .8666 so if pulling 100# tension, only realize 86.66 on pulley
>>and 50# pulling across cuz SINE(sin) is. 5. ( i think riggers and climbers should be familiar with benchmark sine/cosines of 0,15,30,45,90)
So can say, each leg of load pull adds it's cosine x rope tension as a pull against load .
>>we assUme each leg is 0degrees deflection and that that cosine is the 1.0 we assUme
note:on spread to 2 points, only look at half the spread as the angle of deflection for each pull/support
.
Once grasp that, same math for hanging picture with 2 spread anchors on picture and 1 nail in wall
>>the tension on wire is raised so has enough inline force /cosine to pull up on picture
>>incurring the sine as tax for business at that angle
>>this tax can sidewards pull anchors off picture from sine forces produced.
.
my mnemonic:
so politically speaking: Don't let your SIN corrupt your COS(cause)!
.
time to clock in!