Update Content - 2024-12-17

content/zettels/transconductance_amplifiers.md

@@ -56,7 +56,7 @@ Such amplifier is used to control motors (e.g. voice coil, BLDC, stepper motors,
 
 ## Required properties {#required-properties}
 
-Main required properties are (taken from <schmidt20_desig_high_perfor_mechat_third_revis_edition>):
+Main required properties are (taken from (<a href="#citeproc_bib_item_2">Schmidt, Schitter, and Rankers 2020</a>)):
 
 -   **Power delivery capability**
 -   **Dynamic properties**
@@ -211,9 +211,9 @@ W_stop = 0.0025 [W]
 
 ### Howland Current Sources {#howland-current-sources}
 
-See Section 4.2.5 in <&horowitz15_art_of_elect_third_edition>.
+See Section 4.2.5 in (<a href="#citeproc_bib_item_1">Horowitz 2015</a>).
 
-Howland current source is shown in Figure <fig:art_electronics_current_source>.
+Howland current source is shown in [Figure 1](#figure--fig:art-electronics-current-source).
 
 > The output current is sourced through a sense resistor \\(R\_s\\) whose value you can choose independently of the matched resistor array (with resistor pairs \\(R\_1\\) and \\(R\_2\\)).
 > The best way to understand this circuit is to think of \\(IC\_1\\) as a difference amplifier whose output sense and reference connections sample the drop across \\(R\_s\\) (i.e., the current); the latter is buffered by follower IC2 so there is no current error.
@@ -342,4 +342,7 @@ In = 2.4e-06 [A/sqrt(Hz)]
 
 ## Bibliography {#bibliography}
 
-<./biblio/references.bib>
+<style>.csl-entry{text-indent: -1.5em; margin-left: 1.5em;}</style><div class="csl-bib-body">
+  <div class="csl-entry"><a id="citeproc_bib_item_1"></a>Horowitz, Paul. 2015. <i>The Art of Electronics - Third Edition</i>. New York, NY, USA: Cambridge University Press.</div>
+  <div class="csl-entry"><a id="citeproc_bib_item_2"></a>Schmidt, R Munnig, Georg Schitter, and Adrian Rankers. 2020. <i>The Design of High Performance Mechatronics - Third Revised Edition</i>. Ios Press.</div>
+</div>