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return new Lab(o.l, Math.cos(h) * o.c, Math.sin(h) * o.c, o.opacity); cosh = Math.cos(h),

return new Lab(o.l, Math.cos(h) * o.c, Math.sin(h) * o.c, o.opacity); cosh = Math.cos(h),

var c = Math.cos( angle ), s = Math.sin( angle ); var a = Math.cos( x ), b = Math.sin( x );

...a _{inc}} - {Z_1}\cos {\theta _{trn}}}}{{{Z_2}\cos {\theta _{inc}} + {Z_1}\cos {\theta _{trn}}}}$$</p> ...(r\cos \theta - ct)}} = A\sum\limits_{m = 0}^\infty {(2m + 1){i^m}{P_m}(\cos \theta ){j_m}(kr){e^{ - 2\pi ivt}}}$$

...gularScale(t[0])+e.orientation)*Math.PI/180;return{r:n,t:i}}(o),i=n.r*Math.cos(n.t),a=n.r*Math.sin(n.t),{x:i,y:a});return"translate("+[s.x,s.y]+")"}})};va

...gularScale(t[0])+e.orientation)*Math.PI/180;return{r:n,t:i}}(o),i=n.r*Math.cos(n.t),a=n.r*Math.sin(n.t),{x:i,y:a});return"translate("+[s.x,s.y]+")"}})};va

...r)}function ft(t,e,r){return isNaN(t)&&(t=0),isNaN(e)&&(e=0),new dt(r,Math.cos(t*=Ho)*e,Math.sin(t)*e)}function dt(t,e,r){return this instanceof dt?(this. ...n(t){return function(e){return Math.pow(e,t)}}function Cn(t){return 1-Math.cos(t*Vo)}function Dn(t){return Math.pow(2,10*(t-1))}function zn(t){return 1-Ma

<em>&Delta;P = 2&sdot;&sigma;&sdot;cos&theta;/R</em><br> <em>h = 2&sdot;&sigma;&sdot;cos&theta;/&rho;&sdot;g&sdot;R</em><br>

...eOutSine:function(x){return sin(x*PI/2)},easeInOutSine:function(x){return-(cos(PI*x)-1)/2},easeInExpo:function(x){return x===0?0:pow(2,10*x-10)},easeOutEx

...eOutSine:function(x){return sin(x*PI/2)},easeInOutSine:function(x){return-(cos(PI*x)-1)/2},easeInExpo:function(x){return x===0?0:pow(2,10*x-10)},easeOutEx

...World);O.direction.sub(c);O.direction.transformDirection(h);O.coneCos=Math.cos(w.angle); O.penumbraCos=Math.cos(w.angle*(1-w.penumbra));O.decay=0===w.distance?0:w.decay;if(O.shadow=w.cast

...heta - {\theta _0})}^2}} + \sum\limits_{dihedral} {\frac{{{K_\phi }[1 + \cos (n\phi - {\phi _0})]}}{2}} \\ + \sum\limits_{impr} {\frac{{{K_\chi }[1 + \cos (n\chi - {\chi _0})]}}{2}} + \sum\limits_{nobond} {{\varepsilon _{ij}}\le

$$|x_1-x_2|=\sqrt{x_1^2+x_2^2-2|x_1||x_2|\cos(x_1,x_2)}\,,\,\,x_1,x_2\in R^n$$ $$|x_1-x_2| = \sqrt{1+1-2\cos(x_1,x_2)}\,,\,\,x_1,x_2\in R^n, |x_1|=|x_2|=1$$

$$|x_1-x_2|=\sqrt{x_1^2+x_2^2-2|x_1||x_2|\cos(x_1,x_2)}\,,\,\,x_1,x_2\in R^n$$ $$|x_1-x_2| = \sqrt{1+1-2\cos(x_1,x_2)}\,,\,\,x_1,x_2\in R^n, |x_1|=|x_2|=1$$

$$|x_1-x_2|=\sqrt{x_1^2+x_2^2-2|x_1||x_2|\cos(x_1,x_2)}\,,\,\,x_1,x_2\in R^n$$ $$|x_1-x_2| = \sqrt{1+1-2\cos(x_1,x_2)}\,,\,\,x_1,x_2\in R^n, |x_1|=|x_2|=1$$

<p>Handsome, cos why not.</p>

...c Specialist (WFO), Chinese Society of Stomatology orthodontic specialist (COS), Invisible Global Certified Physician, Insignia Global Certified Physician

...ression and replication in cell lines expressing the large T antigen (e.g. COS-7 and 293T cells). They will not replicate episomally in the absence of the

...hedral}}}\sum_n^{n_{\mathrm{i},\mathrm{max}}}(\frac{V_{i,n}}{2})[1+\mathrm{cos}(n_i-\gamma_{i,n})]

// using small-angle approximation cos(x/2) = 1 - x^2 / 8