<rss xmlns:atom="http://www.w3.org/2005/Atom" version="2.0"><channel><title>Physics - Tag - Jorgen Bergstrom</title><link>https://bergstrom.org/tags/physics/</link><description>Physics - Tag - Jorgen Bergstrom</description><generator>Hugo -- gohugo.io</generator><language>en-us</language><copyright>Jorgen Bergstrom</copyright><lastBuildDate>Sat, 25 May 2024 00:00:00 -0500</lastBuildDate><atom:link href="https://bergstrom.org/tags/physics/" rel="self" type="application/rss+xml"/><item><title>Physics Calculation of Hammer Throw Distance with Air Drag</title><link>https://bergstrom.org/posts/hammer_distance_with_drag/</link><pubDate>Sat, 25 May 2024 00:00:00 -0500</pubDate><author>Jorgen Bergstrom</author><guid>https://bergstrom.org/posts/hammer_distance_with_drag/</guid><description>Physics-Based Theory and Numerical Implementation The weight of the hammer ball is 7.26 kg, the material is steel and therefore the ball radius is given by $r = (3m/(4\pi \rho_s))^{1/3}$. The drag force from the air resistance is $F_d = \rho_a v^2 C_d A$, where $A$ is the cross-sectional area. In summary, Newton’s equation in the horizontal and vertical directions can be written in incremental form: $$ \displaystyle \Delta v_x = – \frac{F_d(v)}{m} \frac{v_x}{v} \Delta t$$ $$ \displaystyle \Delta v_y = – \left[ \frac{F_d(v)}{m} \frac{v_y}{v} + g \right] \Delta t$$</description></item></channel></rss>