From 17f37319003e4c55685001024dec2dadaf045a2e Mon Sep 17 00:00:00 2001 From: Peter Sharpe Date: Tue, 30 Jan 2024 01:46:01 -0500 Subject: [PATCH] docs --- ... - The AeroSandbox Dynamics Stack without Optimization.ipynb | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/tutorial/03 - Trajectory Optimization and Optimal Control/03 - The AeroSandbox Dynamics Stack/07 - The AeroSandbox Dynamics Stack without Optimization.ipynb b/tutorial/03 - Trajectory Optimization and Optimal Control/03 - The AeroSandbox Dynamics Stack/07 - The AeroSandbox Dynamics Stack without Optimization.ipynb index 2f96b76b..e7afcd26 100644 --- a/tutorial/03 - Trajectory Optimization and Optimal Control/03 - The AeroSandbox Dynamics Stack/07 - The AeroSandbox Dynamics Stack without Optimization.ipynb +++ b/tutorial/03 - Trajectory Optimization and Optimal Control/03 - The AeroSandbox Dynamics Stack/07 - The AeroSandbox Dynamics Stack without Optimization.ipynb @@ -421,7 +421,7 @@ "source": [ "Looking at these charts, the answer's a bit more obvious: the balloon simply pops, since it is not infinitely elastic and the radius cannot grow to over a kilometer.\n", "\n", - "There is also a second-order effect here that we have ignored: the tension in the balloon skin leads to unequal pressures on the inside and outside of the balloon. This causes the helium to have a slightly higher density than it otherwise would at ambient pressure, which leads to a slightly lower buoyancy force." + "There is also a second-order effect here that we have ignored: the tension in the balloon skin leads to unequal pressures on the inside and outside of the balloon. This causes the helium to have a slightly higher density than it otherwise would at ambient pressure, which leads to a slightly lower buoyancy force. Depending on assumptions about balloon tension, this effect could cause the altitude of the balloon to asymptote to a constant value, rather than increase indefinitely." ], "metadata": { "collapsed": false