Rectangular Cross Section
$b$ | : Width of rectangular section |
$h$ | : Height of rectangular section |
$M$ | : Bending moment |
$x$ | : Distance from compression edge to neutral axis |
$d$ | : Effective depth (distance from compressive edge to tensile re-bar) |
$d_c$ | : Distance from compressive edge to compressive re-bar |
$c$ | : Distance from gravity center of the section to tensile re-bar |
$c_{c}$ | : Distance from gravity center of the section to compressive re-bar |
$\sigma_{c}$ | : Compressive stress of Concrete |
$\sigma_{st}$ | : Tensile stress of Tensile re-bar |
$\sigma_{sc}$ | : Compressive stress of Compressive re-bar |
$n$ | : Ratio of elastic moduluses of rebar and concrete (=15) |
$A_{st}$ | : Total section area of tensile re-bars |
$A_{sc}$ | : Total section area of compressive rebars |
Single Reinforcing Rectangular Section under Bending Moment
\begin{equation} x=\cfrac{n A_{st}}{b} \left[-1+\sqrt{1+\cfrac{2 b d}{n A_{st}}} \right] \end{equation} \begin{equation} \sigma_c=\cfrac{2 M}{b x \left(d-\cfrac{x}{3}\right)} \end{equation} \begin{equation} \sigma_{st}=\cfrac{M}{A_{st} \left(d-\cfrac{x}{3}\right)}=n \sigma_c \cfrac{d-x}{x} \end{equation}Double reinforcing rectangular section under bending moment
\begin{equation} x=-n\cfrac{A_{st}+A_{sc}}{b}+\sqrt{\left[\cfrac{n (A_{st}+A_{sc})}{b}\right]^2+\cfrac{2 n}{b} (d A_{st} + d_c A_{sc})} \end{equation} \begin{equation} \sigma_c=\cfrac{M}{\cfrac{b x}{2} \left(d-\cfrac{x}{3}\right) + n A_{sc} \cfrac{x-d_c}{x}(d-d_c)} \end{equation} \begin{equation} \sigma_{st}=n \sigma_c \cfrac{d-x}{x} \end{equation} \begin{equation} \sigma_{sc}=n \sigma_c \cfrac{x-d_c}{x} \end{equation}Shearing Stress of Concrete and Required Section Area of Stirrup in Rectangular Cross Section
$S$ | : Shearing force |
$\tau_c$ | : Shearing stress of concrete |
$\tau_{ca}$ | : Allowable shearing stress of concrete |
$\sigma_{sa}$ | : Allowable stress of re-bar |
$s$ | : Installation interval of stirrup |
$V_s$ | : Shearing force shared by stirrup |
$A_v$ | : Required section area of stirrup |
Shearing Stress of Concrete and Normal Stress of Re-bar due to Torsional Moment
(Source: Specifications for Highway Bridges, Part III Concrete Bridges, Japan Road Association)
Shearing stress of concrete due to torsional moment
$M_T$ | : Tortional moment |
$\tau_t$ | : Shearing stress of concrete due to torsional moment |
$K_t$ | : Coefficient for stress calculation |
$b$ | : Shorter side of cross section without covers of both sides |
$h$ | : Longer side of cross section without covers of both sides |
At the center of longer side
\begin{equation} K_t=\cfrac{b^2 \cdot h}{\eta_1} \end{equation}At the center of shorter side
\begin{equation} K_t=\cfrac{b^2 \cdot h}{\eta_1 \cdot \eta_2} \end{equation}$h/b$ | 1 | 2 | 3 | 5 | 10 | 20 | $\infty$ |
---|---|---|---|---|---|---|---|
$\eta_1$ | 4.80 | 4.07 | 3.74 | 3.43 | 3.20 | 3.10 | 3.00 |
$\eta_2$ | 1.000 | 0.795 | 0.753 | 0.743 | 0.742 | 0.742 | 0.742 |
Normal stress of re-bars due to torsional moment
$\sigma_{stl}$ | : Stress of lateral re-bar (stirrup) due to torsional moment |
$\sigma_{sta}$ | : Stress of axial re-bar due to torsional moment |
$a$ | : Instalation interval of lateral re-bar (stirrup) |
$A_{wt}$ | : Section area of one lateral re-bar with installation interval $a$ |
$A_{lt}$ | : Total section area of axial re-bars for torsional moment |
$b_t$ | : Width of cross section without covers of both sides |
$h_t$ | : Height of cross section without covers of both sides |
Double Reinforcing Rectangular Section under Compressive Axial force and Bending Moment
\begin{equation} e=M/N \qquad N \text{: Compressive axial force} \end{equation} \begin{align} &x^3-x^2\cdot 3\left(\cfrac{h}{2}-e\right)+x\cdot\cfrac{6n}{b}[A_{st} (e+c)+A_{sc} (e-c_{c})] \\ &-\cfrac{6n}{b}\left[A_{st} \left(c+\cfrac{h}{2}\right)(e+c)+A_{sc} \left(\cfrac{h}{2}-c_{c}\right)(e-c_{c})\right] =0 \end{align} \begin{equation} \sigma_c=\cfrac{M}{\cfrac{b x}{2}\left(\cfrac{h}{2}-\cfrac{x}{3}\right)+\cfrac{n A_{sc}}{x} c_{c} \left(c_{c}-\cfrac{h}{2}+x\right)+\cfrac{n A_{st}}{x} c \left(c+\cfrac{h}{2}-x\right)} \end{equation} \begin{equation} \sigma_{st}=\cfrac{n \sigma_c}{x} \left(c+\cfrac{h}{2}-x\right) \end{equation} \begin{equation} \sigma_{sc}=\cfrac{n \sigma_c}{x} \left(c_{c}-\cfrac{h}{2}+x\right) \end{equation}Double Reinforceing Rectangular Section under Tensile Axial force and Bending Moment
\begin{equation} e=M/N \qquad N \text{: Tensile axial force} \end{equation} \begin{align} &x^3-x^2\cdot 3\left(\cfrac{h}{2}+e\right)-x\cdot\cfrac{6n}{b}[A_{st} (e-c)+A_{sc} (e+c_{c})] \\ &+\cfrac{6n}{b}\left[A_{st} \left(c+\cfrac{h}{2}\right)(e-c)+A_{sc} \left(\cfrac{h}{2}-c_{c}\right)(e+c_{c})\right] =0 \end{align} \begin{align} \sigma_c&=\cfrac{M}{\cfrac{b x}{2}\left(\cfrac{h}{2}-\cfrac{x}{3}\right)+\cfrac{n A_{sc}}{x} c_{c} \left(c_{c}-\cfrac{h}{2}+x\right)+\cfrac{n A_{st}}{x} c \left(c+\cfrac{h}{2}-x\right)} \\ &=\cfrac{N}{\cfrac{n A_{st}}{x}\left(c+\cfrac{h}{2}-x\right)-\cfrac{n A_{sc}}{x} \left(c_{c}-\cfrac{h}{2}+x\right)-\cfrac{b x}{2}} \end{align} \begin{equation} \sigma_{st}=\cfrac{n \sigma_c}{x} \left(c+\cfrac{h}{2}-x\right) \end{equation} \begin{equation} \sigma_{sc}=\cfrac{n \sigma_c}{x} \left(c_{c}-\cfrac{h}{2}+x\right) \end{equation}Concrete and Re-bar Stresses of Circular Cross Section Column
$r$ | : Radius of circular cross section |
$r_s$ | : Location of re-bars in radial direction |
$M$ | : Bending moment |
$N$ | : Axial force |
$\sigma_c$ | : Compressive stress of Concrete |
$\sigma_{st}$ | : Tensile stress of re-bar |
$\sigma_{sc}$ | : Compressive stress of re-bar |
$n$ | : Ratio of elastic moduluses of rebar and concrete (=15) |
$A_{s}$ | : Total section area of re-bars |
$\alpha$ | : Location of neutral axis in radian ($0 < \alpha < \pi$) |
Full compressive section
\begin{equation} A_i=\pi r^2 + n A_s \qquad I_i=\cfrac{\pi r^4}{4}+\cfrac{n A_s r_s^2}{2} \end{equation} \begin{align} &\text{Concrete stresses} & &\sigma_{c1}=\cfrac{N}{A_i}+\cfrac{M}{I_i}\cdot r & &\sigma_{c2}=\cfrac{N}{A_i}-\cfrac{M}{I_i}\cdot r \\ &\text{Re-bar stresses} & &\sigma_{s1}=\cfrac{n r_s}{r}\cdot\sigma_{c1} & &\sigma_{s2}=\cfrac{n r_s}{r}\cdot\sigma_{c2} \\ \end{align}Not full compressive section
Using following equation, $\alpha$ can be calculated by Bisection method.
\begin{equation} e=M/N \end{equation} \begin{equation} \cfrac{e}{r}=\cfrac{\cfrac{\sin 4\alpha}{32}+\cfrac{\pi-\alpha}{8}+\cfrac{\sin^3\alpha\cdot\cos\alpha}{3}+\cfrac{n A_{s}}{4 r^2}\left(\cfrac{r_s}{r}\right)^2} {\cfrac{\sin^3\alpha}{3}+\cfrac{\sin\alpha\cdot\cos^2\alpha}{2}+\cfrac{(\pi-\alpha)\cos\alpha}{2}+\cfrac{n A_{s} \cos\alpha}{2 r^2}} \end{equation}After getting $\alpha$, concrete stress and re-bar stress can be calculated using following equations.
\begin{equation} \sigma_c=\cfrac{M (1+\cos\alpha)}{2 r^3 \left\{\cfrac{\sin 4\alpha}{32}+\cfrac{\pi-\alpha}{8}+\cfrac{\sin^3\alpha\cdot\cos\alpha}{3}\right\}+\cfrac{n A_{s} r_s^2}{2 r}} \end{equation} \begin{align} &\sigma_{st}=n \sigma_c \cfrac{\cfrac{r_s}{r}-\cos\alpha}{1+\cos\alpha} \\ &\sigma_{sc}=n \sigma_c - \cfrac{\sigma_{st}+n \sigma_c}{r+r_s}(r-r_s) \end{align}Checking of $\alpha$ value
\begin{equation} \cos\alpha=\cfrac{n \cfrac{r_s}{r}-\cfrac{\sigma_{st}}{\sigma_c}}{\cfrac{\sigma_{st}}{\sigma_c}+n} \end{equation}Shearing stress of concrete and requied section area of shear re-bar will be calculated using a square cross section model with equivalent cross section area to the circular cross section.