$$\overline{a}\ =\ \frac{\Delta v}{\Delta t}$$

(a)  

$$v=v_i+at$$

(a)  

$$\omega=\omega_i+\alpha t$$

(a)  

$$\Delta x=\left(\frac{v_f+v_i}{2}\right)t$$

(a)  

$$\Delta\theta=\left(\frac{\omega_f+\omega_i}{2}\right)t$$

(a)  

$$\Delta x=v_it\ +\frac{1}{2}at^2$$

(a)  

$$\Delta\theta=\omega_it\ +\frac{1}{2}\alpha t^2$$

(a)  

$$v_f^2=v_i^2+2a\Delta x$$

(a)  

$$\omega_f^2=\omega_i^2+2\alpha\Delta\theta$$

(a)  

$$F_{net}\ =\ ma$$

(a)  

$$w\ =\ mg$$

(a)  

$$μ_s=\frac{F_r}{F_N}$$

(a)  

$$\rho\ =\ \frac{m}{V}$$

(a)  

$$L\ =\ I\omega$$

(a)  

$$KE_{rot}\ =\ \frac{1}{2}I\omega^2$$

(a)  

$$μ_k=\frac{F_f}{F_N}$$

(a)  

$$F\ =\ -k\Delta x$$

(a)  

$$S\ =\ \Delta\theta\cdot r$$

(a)  

$$\omega\ =\ \frac{\Delta\theta}{t}$$

(a)  

$$v\ =\ r\omega\$$

(a)  

$$F_c=ma_c\ =\ \frac{mv^2}{r}\ =\ mr\omega^2$$

(a)  

$$a_c=\frac{v^2}{r}$$

(a)  

$$\alpha\ =\ \frac{\Delta\omega}{\Delta t}$$

(a)  

$$F\ =\ G\frac{m_1m_2}{r^2}$$

(a)  

$$g=\ \frac{GM}{r^2}$$

(a)  

$$W\ =\ fd\cos\theta$$

(a)  

$$KE\ =\ \frac{1}{2}mv^2$$

(a)  

$$PE_g=mgh$$

(a)  

$$KE_i+PE_i\ \left(+W_{nc}\right)\ =\ KE_f+PE_f$$

(a)  

$$P\ =\ \frac{W}{t}$$

(a)  

$$p\ =\ mv$$

(a)  

$$\Delta p\ =\ F_{net}\Delta t$$

(a)  

$$\tau\ =\ rF\sin\theta$$

(a)  

$$a_t\ =\ \frac{\Delta v}{\Delta t}=r\alpha$$

(a)  

$$\tau_{net}\ =I\alpha$$

(a)  

$$I\ =\ MR^2$$

(a)  

$$Q=\frac{V}{t}$$

(a)  

$$Q=mC\Delta T$$

(a)  

$$Q=mL_f$$

(a)  

$$Q=mL_v$$

(a)  

$$W\ =\ P\Delta V$$

(a)  

$$W\ =0$$

(a)  

$$Q\ =\ W$$

(a)  

$$Q\ =\ 0$$

(a)  

$$f\ =\ \frac{1}{T}$$

(a)  

$$v\ =\ \frac{\lambda}{T}\ =\ f\lambda$$

(a)  

$$U_s\ =\ \frac{1}{2}kx^2$$

(a)  

$$T\ =\ 2\pi\sqrt{\frac{m}{k}}$$

(a)  

$$x\left(t\right)=X\cos\left(\frac{2\pi t}{T}\right)$$

(a)  

$$T\ =\ 2\pi\sqrt{\frac{L}{g}}$$

(a)  

$$f_B\ =\ \left|f_1-f_2\right|$$

(a)  

$$f_n=n\left(\frac{v}{2L}\right)$$

(a)  

$$f_n=n\left(\frac{v}{4L}\right)$$

(a)  

$$F\ =\ k\ \frac{\left|q_1q_2\right|}{r^2}$$

(a)  

$$E\ =\ \frac{F}{q}$$

(a)  

$$V\ =\ IR$$

(a)  

$$R\ =\ \frac{\rho L}{A}$$

(a)  

$$P\ =\ IV\ =\ \frac{V^2}{R}\ =\ I^2R$$

(a)  

$$R_s\ =\ R_1+R_2+R_3\ +.\ .\ .$$

(a)  

$$\frac{1}{R_p}=\ \frac{1}{R_1}+\frac{1}{R_2}+\frac{1}{R_3}+\ .\ .\ .$$

(a)  

$$F\ =\ qvB\sin\theta$$

(a)  

$$c\ =\ f\lambda$$

(a)