Duration: 8:42

0 views

0

At \( t=0 \) a charge \( q \) is at the origin and moving in the \( y \)-direction with velocity \( \vec{v}=v \hat{j} \). The charge moves in a magnetic field that is for \( y0 \) out of page and given by \( B_{1} \hat{z} \) and for \( y0 \) into the page and given \( -B_{2} \hat{z} \). The charges subsequent trajectory is shown in the sketch. From this information, we can deduce that
(a) \( q0 \) and \( \left|B_{1}\right|\left|B_{2}\right| \)
(b) \( q0 \) and \( \left|B_{1}\right|\left|B_{2}\right| \)
(c) \( q0 \) and \( \left|B_{1}\right|\left|B_{2}\right| \)
(d) \( q0 \) and \( \left|B_{1}\right|\left|B_{2}\right| \)
📲PW App Link - https://bit.ly/YTAI_PWAP
🌐PW Website - https://www.pw.live