r = 1 2 − sin x r=\frac{1}{2-\sin{x}} r = 2 − s i n x 1 (1)
r 2 d x d t = 4 r^2\frac{dx}{dt}=4 r 2 d t d x = 4 (2)
(i)
r d x d t = 4 r = 4 ( 2 − sin x ) r\frac{dx}{dt}=\frac{4}{r}=4(2-\sin{x}) r d t d x = r 4 = 4 ( 2 − sin x )
(ii)
d r d t = d r d x d x d t = \frac{dr}{dt}=\frac{dr}{dx}\frac{dx}{dt}= d t d r = d x d r d t d x =
= ( − 1 ) ( − cos x ) ( 2 − sin x ) 2 ∗ 4 ( 2 − sin x ) 2 = 4 cos x =\frac{(-1)(-\cos{x})}{(2-\sin{x})^2}*4(2-\sin{x})^2=4\cos{x} = ( 2 − s i n x ) 2 ( − 1 ) ( − c o s x ) ∗ 4 ( 2 − sin x ) 2 = 4 cos x
− 1 ⩽ − sin x ⩽ 1 -1\leqslant-\sin{x}\leqslant1 − 1 ⩽ − sin x ⩽ 1
1 ⩽ 2 − sin x ⩽ 3 1\leqslant2-\sin{x}\leqslant3 1 ⩽ 2 − sin x ⩽ 3
1 ⩾ 1 2 − sin x ⩾ 1 3 1\geqslant\frac{1}{2-\sin{x}}\geqslant\frac{1}{3} 1 ⩾ 2 − s i n x 1 ⩾ 3 1
1 3 ⩽ r ⩽ 1 \frac{1}{3}\leqslant r \leqslant 1 3 1 ⩽ r ⩽ 1
(iii)
v − s p e e d ( v e l o c i t y ) v - speed(velocity) v − s p ee d ( v e l oc i t y )
v = v r 2 + v x 2 = ( d r d t ) 2 + ( r d x d t ) 2 = v=\sqrt{v_r^2+v_x^2}=\sqrt{(\frac{dr}{dt})^2+(r\frac{dx}{dt})^2}= v = v r 2 + v x 2 = ( d t d r ) 2 + ( r d t d x ) 2 =
= 16 cos 2 x + 16 ( 2 − sin x ) 2 = =\sqrt{16\cos^2{x}+16(2-\sin{x})^2}= = 16 cos 2 x + 16 ( 2 − sin x ) 2 =
= 16 + 16 ∗ 4 − 64 sin x = 80 − 64 sin x =\sqrt{16+16*4-64\sin{x}}=\sqrt{80-64\sin{x}} = 16 + 16 ∗ 4 − 64 sin x = 80 − 64 sin x
v ( x = 0 ) = 80 = 4 5 v(x=0)=\sqrt{80}=4\sqrt{5} v ( x = 0 ) = 80 = 4 5
(iv)
a − a c c e l e r a t i o n a- acceleration a − a cce l er a t i o n
a x = r ( d 2 x d t 2 ) 2 + 2 d r d t d x d t = a_x=r(\frac{d^2x}{dt^2})^2+2\frac{dr}{dt}\frac{dx}{dt}= a x = r ( d t 2 d 2 x ) 2 + 2 d t d r d t d x =
= 1 2 − sin x d d t ( 4 ( 2 − sin x ) 2 ) + 2 ∗ 4 cos x ∗ 4 ( 2 − sin x ) 2 = =\frac{1}{2-\sin{x}}\frac{d}{dt}(4(2-\sin{x})^2)+2*4\cos{x}*4(2-\sin{x})^2= = 2 − s i n x 1 d t d ( 4 ( 2 − sin x ) 2 ) + 2 ∗ 4 cos x ∗ 4 ( 2 − sin x ) 2 =
= 4 ∗ 2 ( 2 − sin x ) 2 − sin x ( − cos x ) d x d t + 32 cos x ( 2 − sin x ) 2 = =\frac{4*2(2-\sin{x})}{2-\sin{x}}(-\cos{x})\frac{dx}{dt}+32\cos{x}(2-\sin{x})^2= = 2 − s i n x 4 ∗ 2 ( 2 − s i n x ) ( − cos x ) d t d x + 32 cos x ( 2 − sin x ) 2 =
= ( − 8 ) cos x ∗ 4 ( 2 − sin x ) 2 + 32 cos x ( 2 − sin x ) 2 = 0 =(-8)\cos{x}*4(2-\sin{x})^2+32\cos{x}(2-\sin{x})^2=0 = ( − 8 ) cos x ∗ 4 ( 2 − sin x ) 2 + 32 cos x ( 2 − sin x ) 2 = 0
a r = d 2 r d t 2 − r ( d x d t ) 2 = a_r=\frac{d^2r}{dt^2}-r(\frac{dx}{dt})^2= a r = d t 2 d 2 r − r ( d t d x ) 2 =
= d d t ( 4 cos x ) − 1 2 − sin x ( 4 ( 2 − sin x ) 2 ) 2 = =\frac{d}{dt}(4\cos{x})-\frac{1}{2-\sin{x}}(4(2-\sin{x})^2)^2= = d t d ( 4 cos x ) − 2 − s i n x 1 ( 4 ( 2 − sin x ) 2 ) 2 =
= − 4 sin x d x d t − 16 ( 2 − sin x ) 3 = =-4\sin{x}\frac{dx}{dt}-16(2-\sin{x})^3= = − 4 sin x d t d x − 16 ( 2 − sin x ) 3 =
= − 4 sin x ∗ 4 ( 2 − sin x ) 2 − 16 ( 2 − sin x ) 3 = =-4\sin{x}*4(2-\sin{x})^2-16(2-\sin{x})^3= = − 4 sin x ∗ 4 ( 2 − sin x ) 2 − 16 ( 2 − sin x ) 3 =
= − 16 ( 2 − sin x ) 2 ( sin x + 2 − sin x ) = =-16(2-\sin{x})^2(\sin{x}+2-\sin{x})= = − 16 ( 2 − sin x ) 2 ( sin x + 2 − sin x ) =
= − 32 ( 2 − sin x ) 2 =-32(2-\sin{x})^2 = − 32 ( 2 − sin x ) 2
F = m a F=ma F = ma , so the force acting on P is directed towards the pole