diff --git a/uni/mmme/2xxx/2053_mechanics_of_solids/images/tss4.svg b/uni/mmme/2xxx/2053_mechanics_of_solids/images/tss4.svg new file mode 100644 index 0000000..059c385 --- /dev/null +++ b/uni/mmme/2xxx/2053_mechanics_of_solids/images/tss4.svg @@ -0,0 +1,392 @@ + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + diff --git a/uni/mmme/2xxx/2053_mechanics_of_solids/thermal_stress_and_strain.md b/uni/mmme/2xxx/2053_mechanics_of_solids/thermal_stress_and_strain.md index 8ea0913..43d044d 100755 --- a/uni/mmme/2xxx/2053_mechanics_of_solids/thermal_stress_and_strain.md +++ b/uni/mmme/2xxx/2053_mechanics_of_solids/thermal_stress_and_strain.md @@ -157,6 +157,8 @@ M = \frac{EI}{R} - E\alpha\int_A\Delta Ty\mathrm{d}a \label{eqn:tss-me2} # Thin Walled Cylinders +![](./images/tss4.svg) + - often temperature variations can be approximated as linear through their thickness: $$\Delta T(y) = \Delta T_\text{wall}\frac{y}{t}$$