Change APA force notation from "tau" to "f"

This commit is contained in:
Thomas Dehaeze 2025-02-12 09:53:03 +01:00
parent f40c33d702
commit 80a99f9d22
9 changed files with 78 additions and 60 deletions

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@ -1381,8 +1381,8 @@ The model of the amplified piezoelectric actuator is shown in Figure ref:fig:tes
It can be decomposed into three components: It can be decomposed into three components:
- the shell whose axial properties are represented by $k_1$ and $c_1$ - the shell whose axial properties are represented by $k_1$ and $c_1$
- the actuator stacks whose contribution to the axial stiffness is represented by $k_a$ and $c_a$. - the actuator stacks whose contribution to the axial stiffness is represented by $k_a$ and $c_a$.
The force source $\tau$ represents the axial force induced by the force sensor stacks. The force source $f$ represents the axial force induced by the force sensor stacks.
The sensitivity $g_a$ (in $N/m$) is used to convert the applied voltage $V_a$ to the axial force $\tau$ The sensitivity $g_a$ (in $N/m$) is used to convert the applied voltage $V_a$ to the axial force $f$
- the sensor stack whose contribution to the axial stiffness is represented by $k_e$ and $c_e$. - the sensor stack whose contribution to the axial stiffness is represented by $k_e$ and $c_e$.
A sensor measures the stack strain $d_e$ which is then converted to a voltage $V_s$ using a sensitivity $g_s$ (in $V/m$) A sensor measures the stack strain $d_e$ which is then converted to a voltage $V_s$ using a sensitivity $g_s$ (in $V/m$)

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% Created 2024-11-18 Mon 11:46 % Created 2025-02-12 Wed 09:53
% Intended LaTeX compiler: pdflatex % Intended LaTeX compiler: pdflatex
\documentclass[a4paper, 10pt, DIV=12, parskip=full, bibliography=totoc]{scrreprt} \documentclass[a4paper, 10pt, DIV=12, parskip=full, bibliography=totoc]{scrreprt}
@ -155,7 +155,7 @@ APA 7 & 4.85 & 9.85\\
To compare the stroke of the APA300ML with the datasheet specifications, one side of the APA is fixed to the granite, and a displacement probe\footnote{Millimar 1318 probe, specified linearity better than \(1\,\mu m\)} is located on the other side as shown in Figure \ref{fig:test_apa_stroke_bench}. To compare the stroke of the APA300ML with the datasheet specifications, one side of the APA is fixed to the granite, and a displacement probe\footnote{Millimar 1318 probe, specified linearity better than \(1\,\mu m\)} is located on the other side as shown in Figure \ref{fig:test_apa_stroke_bench}.
The voltage across the two actuator stacks is varied from \(-20\,V\) to \(150\,V\) using a DAC\footnote{The DAC used is the one included in the IO133 card sold by Speedgoat. It has an output range of \(\pm 10\,V\) and 16-bits resolution} and a voltage amplifier\footnote{PD200 from PiezoDrive. The gain is \(20\,V/V\)}. The voltage across the two actuator stacks is varied from \(-20\,V\) to \(150\,V\) using a DAC\footnote{The DAC used is the one included in the IO131 card sold by Speedgoat. It has an output range of \(\pm 10\,V\) and 16-bits resolution} and a voltage amplifier\footnote{PD200 from PiezoDrive. The gain is \(20\,V/V\)}.
Note that the voltage is slowly varied as the displacement probe has a very low measurement bandwidth (see Figure \ref{fig:test_apa_stroke_voltage}). Note that the voltage is slowly varied as the displacement probe has a very low measurement bandwidth (see Figure \ref{fig:test_apa_stroke_voltage}).
\begin{figure}[htbp] \begin{figure}[htbp]
@ -535,8 +535,8 @@ It can be decomposed into three components:
\begin{itemize} \begin{itemize}
\item the shell whose axial properties are represented by \(k_1\) and \(c_1\) \item the shell whose axial properties are represented by \(k_1\) and \(c_1\)
\item the actuator stacks whose contribution to the axial stiffness is represented by \(k_a\) and \(c_a\). \item the actuator stacks whose contribution to the axial stiffness is represented by \(k_a\) and \(c_a\).
The force source \(\tau\) represents the axial force induced by the force sensor stacks. The force source \(f\) represents the axial force induced by the force sensor stacks.
The sensitivity \(g_a\) (in \(N/m\)) is used to convert the applied voltage \(V_a\) to the axial force \(\tau\) The sensitivity \(g_a\) (in \(N/m\)) is used to convert the applied voltage \(V_a\) to the axial force \(f\)
\item the sensor stack whose contribution to the axial stiffness is represented by \(k_e\) and \(c_e\). \item the sensor stack whose contribution to the axial stiffness is represented by \(k_e\) and \(c_e\).
A sensor measures the stack strain \(d_e\) which is then converted to a voltage \(V_s\) using a sensitivity \(g_s\) (in \(V/m\)) A sensor measures the stack strain \(d_e\) which is then converted to a voltage \(V_s\) using a sensitivity \(g_s\) (in \(V/m\))
\end{itemize} \end{itemize}