http://assets.openstudy.com/updates/attachments/569e002de4b0b1fe89e089f2-ganeshie8-1453195319943-zz.png Answer given is 0.6 uN
By symmetry, I thought that the net force is 0. But the textbook says otherwise..
That's correct. The vertical component of the field yields symmetric forces that cancel out. But the radial ones add up to give an upward force of \(2\pi a.i.B\sin \theta\)
that does match with the answer http://www.wolframalpha.com/input/?i=2*pi*1.8%2F100*4.6%2F1000*3.4%2F1000*sin%2820%29
But why \(\mu \times B\) is giving a different answer ? thank you :)
Oh that is for torque experienced by the loop, gotcha !
Then, i guess, the ring experiences both torque and a net force upward
Yes, that's correct! Torque is zero since B is symmetrical about the axis. There is only the upward net force.
I see... but the ring is in MAX potential energy state right ? so if my interpretation is correct, if I slightly tilt the ring, the ring then experiences a torque and rotates by 180 degrees ?
\(B\) and \(\mu\) are almost 180 degrees out of phase in the given diagram..
here is my reasoning: I write the differential force as below: \[d{\mathbf{F}} = \frac{i}{c}d{\mathbf{s}} \times {\mathbf{B}}\] now, I decompose the field as below: \[{\mathbf{B}} = {B_z}{\mathbf{z}} + {B_r}{\mathbf{r}}\] so, after a substitution, I get: \[\begin{gathered} d{\mathbf{F}} = \frac{i}{c}d{\mathbf{s}} \times \left( {{B_z}{\mathbf{z}} + {B_r}{\mathbf{r}}} \right) = \hfill \\ \hfill \\ = \frac{i}{c}d{\mathbf{s}} \times {B_z}{\mathbf{z}} + \frac{i}{c}d{\mathbf{s}} \times {B_r}{\mathbf{r}} \hfill \\ \end{gathered} \]
and the torque here acts to align \(B\) and \(\mu\) I guess
Correct, it means torque is zero, but any slight rotation will create a non zero torque that will increase and flip the ring upside down. It is an unstable state of rotational equilibrium.
Thanks! I guess I am finally getting these :)
now, the first term has a contribute equal to zero, after integration, whereas the contribute of the scond term is: \[F = \frac{{2\pi ia}}{c}B\sin 20\] after integration
I have used the CGS system of units of measures
namely, \(c\) is the speed of light
Oh, I see... it is equivalent to \(dF = i dL\times B\) right ?
yes!
then you're integrating over the circumference of the ring, nice !
Yes, that's the starting point.
yes! Since I have integrate on the differential element \[d{\mathbf{s}}\]
integrated*
the resultant force is vertically directed, upward or downward depending on the orientation of the current
Don't you just apply F = BIL and then take the appropriate component sin(20)? So it is B x I x 2 x pi x r x sin(20) = 6.05 x 10^(-7) N
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