in class 10-28
Equilibrium and Torque
When in static equilibrium, angular acceleration ($\alpha$) is zero; thus, the sum of torques equals zero.
Free body diagrams are expanded to include torques when analyzing systems in equilibrium.
Key Concepts
Static Equilibrium Conditions:
Sum of forces ($\Sigma F = 0$)
Sum of torques ($\Sigma \tau = 0$)
Torque Calculation:
Individual torque ($\tau = r \cdot f_{\perpendicular}$)
$r$ = distance from pivot point
$f_{\perpendicular}$ = perpendicular component of force
Choice of Pivot Points:
Pivot point can be chosen freely; affects torque calculation but not overall equilibrium assessment.
Extended Free Body Diagrams
Represent shapes (e.g., rods) to depict forces acting at specific points.
Important to indicate locations and angles for accurate torque calculations.
Example Problem: Lifting a Heavy Bucket
Bucket of mass 910 kg (weight $W = mg$).
Identify forces acting on the beam and calculate the necessary lift force to maintain equilibrium.
Example Problem: Two Normal Forces at a Support
Analyze normal forces when distributing weight across two support points of a board.
Assign pivot and calculate torques for both ends of the board.
Ladder Problem
For a ladder leaning against a wall:
Forces includes weight, normal forces at contact points, and friction.
Apply conditions for static equilibrium to find the coefficient of static friction needed to prevent slipping.
General Equation:
Coefficient of static friction $\mu_s \geq \frac{1}{2} \tan(\phi)$ (where $\phi$ is the angle).
Important Concepts
Rigid body assumptions: No flexing or bending.
Dynamic vs. Static Analysis: Emphasis on static scenarios makes calculations simpler due to zero angular acceleration conditions.