Theoretical Mechanics IPSP

Jürgen Vollmer, Universität Leipzig

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book:chap3:3.3_newton_s_axioms_and_equations_of_motion_eom

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book:chap3:3.3_newton_s_axioms_and_equations_of_motion_eom [2024/02/01 00:05] – [3.3.5 Self Test] jvbook:chap3:3.3_newton_s_axioms_and_equations_of_motion_eom [2024/02/01 00:13] (current) – fixing typos in mine cart exampe jv
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 \end{align*} \end{align*}
 The mine cart travels with constant velocity $\dot v = 0$, when the attacking forces balance, The mine cart travels with constant velocity $\dot v = 0$, when the attacking forces balance,
-i.e., for $v_c = F_M / m\, \gamma$.+i.e., for $v_c = F_M / \gamma$.
 For a different initial velocity, $v(t_0) = v_0$, one finds an exponential approach to the asymptotic velocity, For a different initial velocity, $v(t_0) = v_0$, one finds an exponential approach to the asymptotic velocity,
 \begin{align*} \begin{align*}
-    v (t) =  v_c + \bigl( v_0 - v_c \bigr) \; \mathrm{e}^{ - \gamma \, (t-t_0) }+    v (t) =  v_c + \bigl( v_0 - v_c \bigr) \; \mathrm{e}^{ - \gamma \, (t-t_0) / m }
 \end{align*} \end{align*}
 After all, After all,
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 and and
 \begin{align*} \begin{align*}
-    \dot v (t) +    m \: \dot v (t) 
-    &= \bigl( v_0 - v_c \bigr) \; (-\gamma) \, \mathrm{e}^{ - \gamma \, (t-t_0) }+    &= \bigl( v_0 - v_c \bigr) \; (-\gamma) \, \mathrm{e}^{ - \gamma \, (t-t_0)/m }
     \\     \\
-    &\bigl( -\gamma \; \bigl( v(t) - v_c \bigr) = -\gamma \; v(t) + F_M \bigr) / m+    &= -\gamma \; \bigl( v(t) - v_c \bigr) = -\gamma \; v(t) + F_M 
 \end{align*} \end{align*}
 </WRAP> </WRAP>
book/chap3/3.3_newton_s_axioms_and_equations_of_motion_eom.1706742301.txt.gz · Last modified: 2024/02/01 00:05 by jv