Bob NH said:
No Dan. The torque wrench applies the measured torque at the square drive of the wrench where it connects to the crow's foot, and it applies a force to the drive point of the crow's foot equal to the force that you pull on the wrench handle. The torque corresponding to the product of that force, times the distance from the crowfoot drive to the center of EMT, is added to the torque measured by the torque wrench.
It will be clear if you draw the force and moment diagram for the point where the torque wrench applies the torque, and then use those forces to calculate the torque applied to the nut.
All right, I'm trying to follow you on this one, Bob. Let's say you've got your crow's foot wrench at the nine o'clock position, as viewed from above, on a nut with a right hand thread. So, your square hole for the torque wrench is at 180 degrees on the cartesian coordinate system I have arbitrarily defined in this system as positive X right, positive Y up. There are several situations I can see on this one.
Assume that
r1 is by definition the mean distance from the square drive of the crow's foot to the center of the crow's foot jaw (i.e. the conduit).
Assume that
r2 is the length of the torque wrench handle from the center of the square drive to the effective position of the electrician's hand.
Assume the electrician always provides force normal to the line defined by
r2.
Situation one: Wrench handle at zero degrees in my defined plane - torque is diminished by r2-r1.
Situation two: Wrench handle at 180 degrees - torque is increased by r2+r1
Any time the variation in torque will be defined by (r1-r2) * the cosine of the angle subtended between
r1 and
r2.
When the wrench is orthogonal to either of these two conditions (cos theda = 0), the resultant torque on the object nut is exactly equal to the applied torque. The applied torque is r times F times sin [angle between
r and
F], always. r is the distance from the center of rotation of the fastener you're twisting to the effective point of where you're making the twisting motion. F is the force you're applying to make something happen. sin theda is the sine of the angle between the radial line passing through the center of "desired" rotation and the vector in line with the force you are applying.
Conclusion: I'm right on only two unique positions out of an infinite number of possibilities. Of the rest of the possibilities, half of the time I'm high, and half of the time I'm low. To correct my original statement, make sure you have the handle of the torque wrench at a 90 degree angle to the line from the middle of the square socket on the crow's foot to the center of the conduit, and you'll not have to compensate for any crow's foot geometry ;-)
An exaggeration to prove the point goes like this. Let's say the crow's foot is of infinite length from the center of the jaws to the center of the square drive. Question: If you apply force on a 3 foot wrench at a 90 degree angle to the line from the center of the jaw to the center of the square drive on that, how much torque are you applying to the nut?
Answer: None. You'll pull the crow's foot straight off the nut.
If you put your wrench handle in line with that infinitely long axis, any force you apply orthogonally will twist the nut right off or on. I think the math still works with realistic dimensions. Thanks for pointing out the error; I only considered the orthogonal axis situation.
It will be clear if you draw the force and moment diagram for the point where the torque wrench applies the torque, and then use those forces to calculate the torque applied to the nut
Yes, you're right. Sorta
||
r X
F|| is by definition r * F * sin theta, right?
Marc, only "spot torque" the biggens.
Edited 09 Nov 2006 - 2239 - Of course, the infinitely long linkage would have to be massless or you wouldn't be able to budge it...