The question asks about the sley velocities and accelerations at the front centre ($0^\circ$) and back centre ($180^\circ$) of a shuttle loom. These represent the endpoints of the sley's reciprocating motion.
At the extreme ends of its travel (front centre and back centre), the sley momentarily stops before reversing direction. In simplified models of such mechanisms, like simple harmonic motion, the velocity at these extreme points is zero.
Therefore, the sley velocities are the same at both positions.
Acceleration is the rate of change of velocity. While the velocity is zero at both extreme points, the sley must change direction rapidly at these points.
Using a simple harmonic motion model $x(t) = A \cos(\omega t)$, velocity is $v(t) = -A \omega \sin(\omega t)$ and acceleration is $a(t) = -A \omega^2 \cos(\omega t)$.
The velocities are the same (zero), but the accelerations have the same magnitude ($A \omega^2$) but opposite directions ($-A \omega^2$ and $A \omega^2$). Thus, the accelerations are different.
Based on the analysis of motion at the extreme points:
This corresponds to Option 1.
Two shuttle looms (A and B), running at same picks per minute, have same mass of sley and associated system for beat up. The crank radius ($r$) and the eccentricity ratio ($e$) of the looms are
$r_A = 10 \text{ cm}; e_A = 0.5; r_B = 6 \text{ cm}; e_B = 0.4$
The ratio of the beat up force of loom A to that of loom B (rounded off to 1 decimal place) is ________
A take-up motion is shown below. The number of teeth on gear A, B, C, D and E are 60, 20, 40, 25 and 50, respectively. The circumference of the take-up roller is 40 cm. If one tooth is broken on gear B, then the wavelength (cm) of the fault in fabric (in integer) is _________________.