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Comment: Migrated to Confluence 5.3

Differential relates the angular positions and forces of three gears on a common axis of rotation. They are commonly used in car steering systems to make sure that when a car rounds a corner, the inside wheel spins less than the outside wheel. In our erg, we use the differential to split an input force from the handle to the two output forces that act on flywheel and the tires.


 
Subscripts

Wiki Markup
{latex} \large L, R, M{latex}
correspond the left half-shaft, right half-shaft, and middle gear, respectively.Three observations:

  •  When we hold the right axle fixed and turn the left axle one revolution, the middle sprocket makes half a revolution in the same angular direction.
  • Holding the middle sprocket in place and turning the left axle one revolution causes the right axle to make one revolution in the opposite direction.
  • The above observations are the same if the left and right axle are switched.

The results can be summarized as such: 

Wiki Markup
{latex}
\large\begin{align*}
\theta_{\text{M}} = \frac{1}{2}\theta_{\text{L}} + \frac{1}{2}\theta_{\text{R}}
\end{align*} 
{latex}

where

Wiki Markup
{latex} \large $\theta$ {latex}
represents angular position. In other words, the position of the middle gear is half the sum of the left and right gears. Say that
Wiki Markup
{latex} \large $\omega$ {latex}
represents angular velocity,
Wiki Markup
{latex} \large $\alpha${latex}
represents angular acceleration, and
Wiki Markup
{latex} \large $\tau$ {latex}
represents torque.
Wiki Markup
{latex} \large $r$ {latex}
is the radius of the gear, and
Wiki Markup
{latex} \large $v$ {latex}
is the linear velocity at the edge of a gear. From the first equation, we can find the relationships between the angular and linear velocities of the gears. 

Wiki Markup
{latex}
\large

\begin{align*}
\omega_{\text{M}} =& \frac{1}{2} \left( \omega_{\text{L}} + \omega_{\text{R}} \right)
\\
\omega_{\text{M}} r_{\text{M}} =& \frac{1}{2} ( \omega_{\text{L}} r_{\text{M}} +
\omega_{\text{R}} r_{\text{M}})
\\
v_{\text{M}} =& \frac{1}{2} \left( \omega_{\text{L}} r_{\text{M}} \frac{r_{\text{L}}}{r_{\text{L}}} +
\omega_{\text{R}} r_{\text{M}} \frac{r_{\text{R}}}{r_{\text{R}}} \right)
\\
v_{\text{M}} =& \frac{1}{2} \left( v_{\text{L}} \frac{r_{\text{M}}}{r_{\text{L}}} +
v_{\text{R}} \frac{r_{\text{M}}}{r_{\text{R}}} \right)
\end{align*}
{latex}

We assume that these ideal gears are frictionless and massless. Therefore, we can use conservation of energy to say that input power equals output power. Say

Wiki Markup
{latex} \large $P$ {latex}
represents power as a function of time.

Wiki Markup
{latex}
\large
\begin{align*}
&P_{\text{M}} = P_{\text{L}} + P_{\text{R}} \\
&\tau_{\text{M}} \cdot \omega_{\text{M}} = \tau_{\text{L}} \cdot \omega_{\text{L}} +
\tau_{\text{R}} \cdot \omega_{\text{R}} \\
&\tau_{\text{M}} \cdot \left[ \frac{1}{2} \left( \omega_{\text{L}} + \omega_{\text{R}} \right) \right]
= \tau_{\text{L}} \cdot \omega_{\text{L}} +
\tau_{\text{R}} \cdot \omega_{\text{R}}
\end{align*}
{latex}

If we consider

Wiki Markup
{latex}\large $\omega_{\text{L}}$ {latex}
and
Wiki Markup
{latex} $\omega_{\text{R}}$ {latex}
separately, we find that

Wiki Markup
{latex}
\large
\begin{align*}
\frac{1}{2} \tau_{\text{M}} \omega_{\text{L}} &= \tau_{\text{L}} \omega_{\text{L}}, \;\;\;
\frac{1}{2} \tau_{\text{M}} \omega_{\text{R}} = \tau_{\text{R}} \omega_{\text{R}}
\\
\frac{1}{2} \tau_{\text{M}} &= \tau_{\text{L}}, \;\;\;\;\;\;\; \;\; \; \;\; \frac{1}{2} \tau_{\text{M}} = \tau_{\text{R}}
\end{align*}
{latex}

Therefore, we can conclude that the relationships between torques is the same as the relationships between angular position; a torque on the middle gear is evenly divided between the torque on the left gear and the torque on the right gear.

Wiki Markup
{latex}
\large
\begin{align*}
\tau_{\text{M}} &= \tau_{\text{L}} + \tau_{\text{R}} \\
\tau_{\text{L}} &= \tau_{\text{R}} = \frac{1}{2} \tau_{\text{M}}
\end{align*}
{latex}
Prof Ruina's favorite video on how a differential works

Widget Connector
urlhttp://www.youtube.com/watch?v=yYAw79386WI