More ring design tutorial devel.

bmad-doc/tutorial_ring_design/doc/macros.tex

@@ -119,6 +119,7 @@
 \newcommand{\ltt}{{\sl Long Term Tracking}\xspace}
 \newcommand{\da}{{\sl Dynamic Aperture}\xspace}
 \newcommand{\sodom}{{\sl SODOM-2}\xspace}
+\newcommand{\spinstrob}{{\sl spin_stroboscope}\xspace}
 \newcommand{\bmad}{{\sl Bmad}\xspace}
 \newcommand{\mad}{{\sl MAD}\xspace}
 \newcommand{\quickplot}{{\sl Quick Plot}\xspace}

bmad-doc/tutorial_ring_design/doc/tutorial_ring_design.tex

@@ -1654,13 +1654,13 @@ \subsection{Example: tao.init for the Tune Cell}
 \begin{code}
 ! Require periodic betas in center FoDo cells of 2 o'clock tune cell
 datum(1) = 'expression: lat::beta.a[QFSS_2##4] - lat::beta.a[QFSS_2##5]' 
- '' '0' 'end' 'target' 0 10
+ '' '' '' 'target' 0 10
 datum(2) = 'expression: lat::beta.b[QFSS_2##4] - lat::beta.b[QFSS_2##5]' 
- '' '0' 'end' 'target' 0 10
+ '' '' '' 'target' 0 10
 datum(3) = 'expression: lat::alpha.a[QFSS_2##4] - lat::alpha.a[QFSS_2##5]' 
- '' '0' 'end' 'target' 0 10
+ '' '' '' 'target' 0 10
 datum(4) = 'expression: lat::alpha.b[QFSS_2##4] - lat::alpha.b[QFSS_2##5]' 
- '' '0' 'end' 'target' 0 10
+ '' '' '' 'target' 0 10
 \end{code}
 
 The syntax \vn{lat::beta.a[QFSS_2\#\#4]} evaluates to the value of the \vn{a}-mode beta function at the fourth lattice element named \vn{QFSS_2}.
@@ -1835,10 +1835,10 @@ \subsection{Example}
  Values at End of Element:
  Index name key ... orbit ... spin 
  ... x ... x 
- 0 BEGINNING Beginning_Ele ... 0.000000E+00 ... 0.000000E+00 
- 1 B Sbend ... 5.027722E-03 ... -1.414516E-01 
- 2 Q Quadrupole ... -1.599068E-02 ... -7.350543E-02 
- 3 END Marker ... -1.599068E-02 ... -7.350543E-02 
+ 0 BEGINNING Beginning_Ele ... 0.000000E+00 ... 1.000000E+00 
+ 1 B Sbend ... 2.888946E-02 ...  9.886413E-01 
+ 2 Q Quadrupole ... -1.847740E-02 ...  9.768026E-01 
+ 3 END Marker ... -1.847740E-02 ...  9.768026E-01 
 \end{code}
 
 or the \vn{show element} command
@@ -1863,7 +1863,7 @@ \subsection{Exercises:}
 
 \begin{enumerate}[leftmargin=*]
 \item {\bf Phase Space:} Construct a lattice with a single drift of 2 meters length.
-Set the particle species to be protons with a reference energy of $10^12$~eV (so the approximation
+Set the particle species to be protons with a reference energy of $10^{12}$~eV (so the approximation
 that the particle velocity is speed of light can be made), and
 Set the initial particle position to have $p_x = 0.2$, $p_z = 1$ with all other coordinates
 zero. Calculate from first principles what the phase space coordinates will be at the end of the
@@ -1988,7 +1988,7 @@ \subsection{Adding RF Cavities}
 
 The example files for this section can be found at \vn{/lattices/9_RF/AddingRF/}
 
-In a real machine, electrons emit synchrotron radiation as they bend around the ring, so we need to replenish the energy with an RF system. Let’s put RF cavities in the 10 o’clock straight section of our ring. We will design a special FODO cellwith RF cavities \vn{FODORF} and replace 4 FODO cells in the 10 o’clock straight section. 
+In a real machine, electrons emit synchrotron radiation as they bend around the ring, so we need to replenish the energy with an RF system. Let’s put RF cavities in the 10 o’clock straight section of our ring. We will design a special FODO cell with RF cavities \vn{FODORF} and replace 4 FODO cells in the 10 o’clock straight section. 
 
 In the ESR, there are two RF cavities of length $4.017 \textrm{m}$ between each quadrupole with equal drift spaces between each element. We will follow these dimensions as shown in Fig.~\ref{f:fodorf}.
 
@@ -2015,7 +2015,7 @@ \subsection{Example: Consturcting the FODO cell with RF cavities}
 FODORF: line = (QFSS, DRF, RF0, DRF, RF0, DRF, QDSS, DRF, RF0, DRF, RF0, DRF)
  \end{code}
 
- \item Replace 4 FODO cells in the 10 o'clock section with \vn{FODORF} by modifying \vn{SEXTANT9} and \vn{SEXTANT9}:
+ \item Replace 4 FODO cells in the 10 o'clock section with \vn{FODORF} by modifying \vn{SEXTANT9} and \vn{SEXTANT11}:
  \begin{code}
 SEXTANT9: line = (4*FODOSSF, SS_TO_ARCF, 20*FODOAF, 
  ARC_TO_SSF, 2*FODOSSF, 2*FODORF)
@@ -2036,7 +2036,7 @@ \subsection{Exercises}
 %
 \item 
 Modify the \vn{lcavity} in the \vn{cavity.bmad} to have a small length (so the transit time is
-small), and set the beginning momentum small enough so the relativistic beta is significantly than
+small), and set the beginning momentum small enough so the relativistic beta is significantly less than
 one. Starting the particle with a finite $z$, calculate the ending $z$ after the cavity and verity
 that the change in $z$ is consistent with what Bmad calculates.
 %
@@ -3214,32 +3214,12 @@ \subsection{Exercises}
 \begin{enumerate}[leftmargin=*]
 %
 \item {\bf Zero orbit at IP:}
-Use 4 horizontal/vertical kickers around the IP (CH/V_104 to CH/V_107, 8 total kickers) to make the orbit exactly 0 at the IP without affecting the rest of the ring.
+Use 4 horizontal/vertical kickers around the IP (CH/V\_104 to CH/V\_107, 8 total kickers) to make the orbit exactly 0 at the IP without affecting the rest of the ring.
 %
 \end{enumerate}
 
 \newpage
 
-%------------------------------------------------------------------------------
-%------------------------------------------------------------------------------
-%\section{Tracking with Ramping and Spin Tracking}
-
-%------------------------------------------------------------------------------
-%\subsection{Tracking with Ramping}
-%The ESR will not be used to accelerate, however to show what ramping in Bmad might look like we include this section.
-
-%------------------------------------------------------------------------------
-%\subsection{Adding Siberian Snakes}
-%Taylor element overview
-
-
-
-%------------------------------------------------------------------------------
-%\subsection{Invariant Spin Field Calculations}
-%\sodom $\rightarrow$ \ltt
-
-%\newpage
-
 %------------------------------------------------------------------------------
 %------------------------------------------------------------------------------
 \appendix

bmad-doc/tutorial_ring_design/lattices/8_PhaseSpace/orbit.bmad

@@ -2,7 +2,7 @@
 beginning[beta_a] = 10. ! m a-mode beta function
 beginning[beta_b] = 10. ! m b-mode beta function
 beginning[e_tot] = 10e6 ! eV
-parameter[geometry] = open ! or closed
+parameter[geometry] = open з! or closed
 bmad_com[spin_tracking_on] = T
 
 particle_start[y] = 0.01