Respuesta :
Answer:
[tex]\frac{m}{r}(v_b^2-v_t^2)+2mg[/tex]
Explanation:
When the ball is at the bottom position of the vertical circle, the forces acting on the ball are:
- The tension in the string, [tex]T_b[/tex], upward
- The weight of the ball, [tex]mg[/tex], downward
The resultant of these forces must be equal to the centripetal force, which points upward as well (towards the center of the circle), so:
[tex]T_b-mg=m\frac{v_b^2}{r}[/tex] (1)
where [tex]v_b[/tex] is the speed of the ball at the bottom of the circle, r the radius of the circle, and m the mass of the ball.
When the ball is at the top position of the vertical circle, the weight still acts downward, however the tension in the string also acts downward, so the equation of the forces becomes:
[tex]T_t+mg=m\frac{v_t^2}{r}[/tex] (2)
where
[tex]T_t[/tex] is the tension in the string in the top position
[tex]v_t[/tex] is the speed of the ball in the top position
By subtracting eq.(2) from eq.(1), we find:
[tex]T_b-mg-(T_t+mg)=m\frac{v_b^2}{r}-m\frac{v_t^2}{r}\\T_b-T_t=\frac{m}{r}(v_b^2-v_t^2)+2mg[/tex]
So, this is the difference in tension between the two positions.
The difference in the magnitude of the tension at the bottom and top is [tex]2mg + \frac{m}{L} (v_b^2 - v_t^2)[/tex]
The given parameters;
- mass of the string, = m
- length of the string, = L
- speed of the string, = v
The tension of the string at the top of the circle;
[tex]T_t = \frac{mv_t^2}{r} - mg[/tex]
The tension of the string at the bottom of the circle;
[tex]T_b = \frac{mv_b^2}{r} + mg[/tex]
The difference in the magnitude of the tension at the bottom and top;
[tex]T_b -T_t = \frac{mv_b^2}{r} + mg - (\frac{mv_t^2}{r} -mg)\\\\T_b -T_t =\frac{mv_b^2}{r} + mg - \frac{mv_t^2}{r} + mg\\\\T_b -T_t = 2mg + \frac{mv_b^2}{r} - \frac{mv_t^2}{r} \\\\T_b -T_t = 2mg + \frac{m}{r} (v_b^2 - v_t^2)\\\\ (r = L)\\\\T_b -T_t = 2mg + \frac{m}{L} (v_b^2 - v_t^2)[/tex]
Thus, the difference in the magnitude of the tension at the bottom and top is [tex]2mg + \frac{m}{L} (v_b^2 - v_t^2)[/tex]
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