| Literature DB >> 35129590 |
Colleen M McDowell1, Krishnakumar Kizhatil2, Michael H Elliott3, Darryl R Overby4, Joseph van Batenburg-Sherwood4, J Cameron Millar5, Markus H Kuehn6, Gulab Zode5, Ted S Acott7, Michael G Anderson8, Sanjoy K Bhattacharya9, Jacques A Bertrand10, Terete Borras11, Diane E Bovenkamp12, Lin Cheng13, John Danias14, Michael Lucio De Ieso15, Yiqin Du16, Jennifer A Faralli17, Rudolf Fuchshofer18, Preethi S Ganapathy19, Haiyan Gong20, Samuel Herberg19, Humberto Hernandez21, Peter Humphries22, Simon W M John23, Paul L Kaufman1, Kate E Keller24, Mary J Kelley25, Ruth A Kelly26, David Krizaj27, Ajay Kumar16, Brian C Leonard28, Raquel L Lieberman29, Paloma Liton30, Yutao Liu31, Katy C Liu32, Navita N Lopez33, Weiming Mao34, Timur Mavlyutov1, Fiona McDonnell32, Gillian J McLellan35, Philip Mzyk1, Andrews Nartey36, Louis R Pasquale37, Gaurang C Patel38, Padmanabhan P Pattabiraman34, Donna M Peters17, Vijaykrishna Raghunathan36, Ponugoti Vasantha Rao39, Naga Rayana34, Urmimala Raychaudhuri40, Ester Reina-Torres10, Ruiyi Ren20, Douglas Rhee41, Uttio Roy Chowdhury42, John R Samples43, E Griffen Samples44, Najam Sharif45, Joel S Schuman46, Val C Sheffield47, Cooper H Stevenson5, Avinash Soundararajan34, Preeti Subramanian12, Chenna Kesavulu Sugali34, Yang Sun48, Carol B Toris49, Karen Y Torrejon50, Amir Vahabikashi51, Janice A Vranka52, Ting Wang34, Colin E Willoughby53, Chen Xin54, Hongmin Yun55, Hao F Zhang56, Michael P Fautsch56, Ernst R Tamm57, Abbot F Clark58, C Ross Ethier59, W Daniel Stamer60.
Abstract
Due to their similarities in anatomy, physiology, and pharmacology to humans, mice are a valuable model system to study the generation and mechanisms modulating conventional outflow resistance and thus intraocular pressure. In addition, mouse models are critical for understanding the complex nature of conventional outflow homeostasis and dysfunction that results in ocular hypertension. In this review, we describe a set of minimum acceptable standards for developing, characterizing, and utilizing mouse models of open-angle ocular hypertension. We expect that this set of standard practices will increase scientific rigor when using mouse models and will better enable researchers to replicate and build upon previous findings.Entities:
Mesh:
Year: 2022 PMID: 35129590 PMCID: PMC8842499 DOI: 10.1167/iovs.63.2.12
Source DB: PubMed Journal: Invest Ophthalmol Vis Sci ISSN: 0146-0404 Impact factor: 4.925
Figure 1.Schematic diagram of outflow pathway and structures in the trabecular meshwork. (A) Schematic diagram depicting conventional and uveoscleral pathway in the anterior eye chamber. (B) A magnified view of trabecular meshwork (TM) depicting distal regions including collector channel entrances (CCEs), collector channels (CCs), episcleral vein (EV), and aqueous vein (AV). CB, ciliary body; SC, Schlemm's canal; IW, inner wall; JCT, juxtacanalicular. Reprinted with permission from Carreon T, van der Merwe E, Fellman RL, Johnstone M, Bhattacharya SK. Aqueous outflow - a continuum from trabecular meshwork to episcleral veins. Prog Retin Eye Res. 2017;57:108–133.
Figure 2.Histogram of measured facilities (C) in wild-type C57BL/6J enucleated mouse eyes. The lognormal distribution is clearly evident. The modal facility value is 3 to 6 nL/min/mmHg. Inset shows the same data, after log transformation. Reprinted with permission from Reina-Torres E, Bertrand JA, O'Callaghan J, Sherwood JM, Humphries P, Overby DR. Reduced humidity experienced by mice in vivo coincides with reduced outflow facility measured ex vivo. Exp Eye Res. 2019;186:107745. © 2019 Elsevier Ltd.
Figure 3.Linearity of pressure–flow rate curve in live mice. (A) C57BL/6J mouse pressure–flow rate curve (N = 6 eyes in situ in live animals; AC perfusion). Over the flow rate range of 100 to 500 nL/min, corresponding to a mean pressure of 15.58 ± 2.83 to 35.18 ± 4.26 mmHg (mean ± square deviation from the mean [SDM]), the curve approached linearity: r2 = 0.9891 ± 0.0076 (mean ± SDM); AIC (two-level linear nested design) = 128.2; AIC (three-level linear nested design) = 130. Computed facility = 19.5 ± 0.8 nL/min/mmHg (mean ± SEM). (B) C57BL/6J mouse pressure–flow rate curve (N = 6 eyes in situ in live animals; PC perfusion). Over the flow rate range of 100 to 500 nL/min, corresponding to a mean pressure of 13.36 ± 2.77 to 33.21 ± 5.57 mmHg (mean ± SDM), the curve approached linearity: r2 = 0.9882 ± 0.0032 (mean ± SDM); AIC (two-level linear nested design) = 156.2; AIC (three-level linear nested design) = 155.9. Computed facility = 21.0 ± 2.1 nL/min/mmHg (mean ± SEM). Reprinted with permission from Lopez NN, Patel GC, Raychaudhuri U, et al. Anterior chamber perfusion versus posterior chamber perfusion does not influence measurement of aqueous outflow facility in living mice by constant flow infusion. Exp Eye Res. 2017;164:95–108. © 2017 Elsevier Ltd.
Figure 4.Examples of appropriate histological examination of the outflow pathway. (A, B) Semithin sections (Richardson's stain) through the iridocorneal angle of representative control and Cav-1 knockout (KO) eyes. The chamber angle is open in control and Cav-1 KO eyes, and obvious abnormalities of the CB, TM, and SC are absent. (C, D) Ultrastructural changes in the JCT region of mice treated with or without dexamethasone (DEX) for 3 to 4 weeks. (C) In sham-treated control mice without DEX, optically open spaces (stars) were often observed between JCT cells with processes extending in many directions. (D) In DEX-treated mice, the JCT was often filled with fine fibrillar material (arrows), and the JCT cells appeared elongated. TL, trabecular lamellae. A and B are reprinted from Elliott MH, Ashpole NE, Gu X, et al. Caveolin-1 modulates intraocular pressure: implications for caveolae mechanoprotection in glaucoma. Sci Rep. 2016;6:37127. C and D are reprinted with permission from Overby DR, Bertrand J, Tektas OY, et al. Ultrastructural changes associated with dexamethasone-induced ocular hypertension in mice. Invest Ophthalmol Vis Sci. 2014;55:4922–4933. © 2014 Association for Research in Vision and Ophthalmology.