5 items with this tag.
C11-E When you put rope material under tension force, and it behaves with tensile-compressive stress there is a relationship, in the formula where [$w$ → When we read this, it is telling us that Downarrow in a more natural way.] is the width of the object, $${\Delta w \over w_0} = -\sigma{\Delta l \...
C11-E The difference between force due to the gravitational interaction about the center of mass, changing the center of gravity… This results in bodies in gravitation tending to “face” one another, due to the torque and rotation matching the rate of revolution.
C11-E Two forces with equal magnitude, and opposite direction, at two different points on a rigid body form a “couple” for example in the case where we’re producing shear stress.
C8-5 Discussion, formula For [$i$ → When we read this, it is telling us that $Delta E_{text{required}} = T cdot Delta S in a more natural way.] particles with masses [$m_i$ → When we read this, it is telling us that $|psi_{text{human}}rangle = sum_i c_i|phi_irangle in a more natural way.] each posit...
C11-4 WaitWhat — are there any elastic modulus under which stress is a vector quantity? GotIt C11-E 11.93 demonstrates finding stress for skew cross-sections, skew force applied.