Step 1: Two ways to increase the force on a current-carrying conductor:
\[ F = BIL \sin\theta \]
where:
\( F \) = force on the conductor, \( B \) = magnetic field strength, \( I \) = current, \( L \) = length of the conductor in the field, \( \theta \) = angle between field and current.
Step 2: Device based on this principle:
The working of an
electric motor depends on the force experienced by a current-carrying conductor in a magnetic field.
Step 3: Fleming’s Left-Hand Rule:
It states that —
“If the forefinger, middle finger, and thumb of the left hand are stretched mutually perpendicular to each other, then —”

Note: The interaction between magnetic field and electric current is the fundamental principle behind all
electromechanical devices such as electric motors, loudspeakers, and galvanometers.
The direction of the force acting on the electron entering perpendicular to the magnetic field as shown in the figure, will be:
Find the unknown frequency if 24 is the median of the following frequency distribution:
\[\begin{array}{|c|c|c|c|c|c|} \hline \text{Class-interval} & 0-10 & 10-20 & 20-30 & 30-40 & 40-50 \\ \hline \text{Frequency} & 5 & 25 & 25 & \text{$p$} & 7 \\ \hline \end{array}\]