\({T_2} = \frac{{2{u_2}\sin ({{90}^o} - \theta )}}{g}\)\( = \frac{{2{u_2}\cos \theta }}{g}\)
\({T_1} = {T_2}\)
\(\Rightarrow \frac{{2{u_1}}}{g} = \frac{{2{u_2}\cos \theta }}{g}\)
\(\Rightarrow {u_1} = {u_2}\cos \theta \)
\({H_1} = \frac{{u_1^2}}{{2g}}\)
\({H_2} = \frac{{u_2^2{{\sin }^2}({{90}^o} - \theta )}}{{2g}}\)
\(\therefore {H_2} = \frac{{u_2^2{{\cos }^2}\theta }}{{2g}}\)
\( \frac{{{H_1}}}{{{H_2}}} = \frac{{u_1^2/2g}}{{u_2^2{{\cos }^2}\theta /2g}}\)= 1 \([\,{u_1} = {u_2}\cos \theta \,]\)
કોલમ $-I$ | કોલમ $-II$ |
$(1)$ કોણીય વેગમાન | $(a)$ અદિશ |
$(2)$ સ્થિતિઊર્જા | $(b)$ સદિશ |
$(c)$ એકમ સદિશ |