If the string tripled in length but the speed of the ball remained the same, show mathematically how the inward force on the ball would change.
3 years ago
You'll need an equation from Kinematics and an equation from Dynamics for this:
$\left|a_c\right|=\frac{v^2}{r}$|ac|=v2r and $F=m\cdot a$F=m·a
In this case, we're replacing that r with L for or original and 3L for our tripled rope length
$a_A=\frac{v^2}{L}$aA=v2L and $a_B=\frac{v^2}{3L}$aB=v23L
Now let's compare what happened between aA and aB:
- our velocities did not change
- our denominator (the radius of the curve traveled by the ball) tripled
If our denominator increases, then our acceleration must have decreased! To prove this, let's substitute aA into our equation for aB
$a_A=\frac{v^2}{L}$aA=v2L and $a_B=\frac{1}{3}\cdot\frac{v^2}{L}$aB=13 ·v2L
$a_B=\frac{1}{3}\cdot a_A$aB=13 ·aA
Now we almost have our solution - let's figure out how this affects our inward force!
$F=m\cdot a$F=m·a
$F_A=m\cdot a_A$FA=m·aA and $F_B=m\cdot\frac{1}{3}\cdot a_A$FB=m·13 ·aA
since the masses have not changed between our two scenarios, the ONLY thing affecting the final force is our changes to the acceleration!
$F_B=\frac{1}{3}F_A$FB=13 FA
3 years ago
Answered By Emily D
You'll need an equation from Kinematics and an equation from Dynamics for this:
$\left|a_c\right|=\frac{v^2}{r}$|ac|=v2r and $F=m\cdot a$F=m·a
In this case, we're replacing that r with L for or original and 3L for our tripled rope length
$a_A=\frac{v^2}{L}$aA=v2L and $a_B=\frac{v^2}{3L}$aB=v23L
Now let's compare what happened between aA and aB:
- our velocities did not change
- our denominator (the radius of the curve traveled by the ball) tripled
If our denominator increases, then our acceleration must have decreased! To prove this, let's substitute aA into our equation for aB
$a_A=\frac{v^2}{L}$aA=v2L and $a_B=\frac{1}{3}\cdot\frac{v^2}{L}$aB=13 ·v2L
$a_B=\frac{1}{3}\cdot a_A$aB=13 ·aA
Now we almost have our solution - let's figure out how this affects our inward force!
$F=m\cdot a$F=m·a
$F_A=m\cdot a_A$FA=m·aA and $F_B=m\cdot\frac{1}{3}\cdot a_A$FB=m·13 ·aA
since the masses have not changed between our two scenarios, the ONLY thing affecting the final force is our changes to the acceleration!
$F_B=\frac{1}{3}F_A$FB=13 FA