big man
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Question:
The link below gives the question I'm interested in. The question is p6.2.
http://www.tkk.fi/Yksikot/Sahkomagnetiikka/kurssit/S-96.1101/harjoitukset/S961101_2006_h07.pdf
My Thoughts
OK, now I thought I knew how to do this question. The expression for the magnetic field shows that it varies with the position along y and varies with time.
So what I thought you'd do is this:
\Phi = \int{B.ds}
Where the differential area is given as:
dS_z=dx dy
So the above integral becomes:
\Phi = b B_0 \int{B.dy}
where b is dx (0.1) and B_0=3 \mu T and B is the rest of the expression for the varying magnetic field.
So I thought you'd integrate this expression with limits of 0 to 0.3, but the answer I get is nothing like their answer??
I end up with an expression for the current i of:
i=- \frac {B_0 b \omega} {R k}[ cos(\omega t -k a)-cos(\omega t)]
This is nothing like their expression of:
i=- \frac {B_0 b \omega} {R k} [sin(\frac {1} {2} k a) sin(\omega t- \frac {1} {2} k a)]
This is simplified by them in the hints section (just scroll down the page to find the hints).
So what am I doing wrong here??
EDIT: oops my expressions for I are meant to contain cosines and not sines.
The link below gives the question I'm interested in. The question is p6.2.
http://www.tkk.fi/Yksikot/Sahkomagnetiikka/kurssit/S-96.1101/harjoitukset/S961101_2006_h07.pdf
My Thoughts
OK, now I thought I knew how to do this question. The expression for the magnetic field shows that it varies with the position along y and varies with time.
So what I thought you'd do is this:
\Phi = \int{B.ds}
Where the differential area is given as:
dS_z=dx dy
So the above integral becomes:
\Phi = b B_0 \int{B.dy}
where b is dx (0.1) and B_0=3 \mu T and B is the rest of the expression for the varying magnetic field.
So I thought you'd integrate this expression with limits of 0 to 0.3, but the answer I get is nothing like their answer??
I end up with an expression for the current i of:
i=- \frac {B_0 b \omega} {R k}[ cos(\omega t -k a)-cos(\omega t)]
This is nothing like their expression of:
i=- \frac {B_0 b \omega} {R k} [sin(\frac {1} {2} k a) sin(\omega t- \frac {1} {2} k a)]
This is simplified by them in the hints section (just scroll down the page to find the hints).
So what am I doing wrong here??
EDIT: oops my expressions for I are meant to contain cosines and not sines.
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