\(\sqrt5 IL\)
5 IL
\(\sqrt3 IL\)
3 IL
The magnetic force \( \vec{F} \) on a wire carrying a current \( I \) of length \( L \) in a magnetic field \( \vec{B} \) is given by the formula: \[ \vec{F} = I (\vec{L} \times \vec{B}) \] where \( \vec{L} \) is the vector representation of the wire's length and direction. For a wire along the positive x-axis, we have \( \vec{L} = L\vec{i} \). Given the magnetic field \( \vec{B} = 2\vec{i} + 3\vec{j} - 4\vec{k} \), we begin by computing the cross product \( \vec{L} \times \vec{B} \): \[ \vec{L} \times \vec{B} = (L\vec{i}) \times (2\vec{i} + 3\vec{j} - 4\vec{k}) \] \[ = L (\vec{i} \times 2\vec{i} + \vec{i} \times 3\vec{j} + \vec{i} \times (-4\vec{k})) \] Since \( \vec{i} \times \vec{i} = 0 \), the remaining cross products are: \[ \vec{i} \times \vec{j} = \vec{k}, \quad \vec{i} \times \vec{k} = -\vec{j} \] Thus, \[ \vec{L} \times \vec{B} = L (0 + 3\vec{k} + 4\vec{j}) = L (4\vec{j} + 3\vec{k}) \] Now calculate the magnitude of the force \( \vec{F} \): \[ |\vec{F}| = I | \vec{L} \times \vec{B} | = I \sqrt{(4L)^2 + (3L)^2} \] \[ = I \sqrt{16L^2 + 9L^2} = I \sqrt{25L^2} = 5IL \] Therefore, the magnitude of the magnetic force acting on the wire is \( 5IL \).
The correct option is (B): 5 IL
\(\vec{F}=I(\vec{l}\times\vec{B})\)
\(I[(L\hat{i})\times(2\hat i+3\hat j-4\hat k)]\)
\(=I(4L\hat j+ 3L\hat k)\)
\(|\vec{F}|=5\,IL\)
A sphere of radius R is cut from a larger solid sphere of radius 2R as shown in the figure. The ratio of the moment of inertia of the smaller sphere to that of the rest part of the sphere about the Y-axis is :
The current passing through the battery in the given circuit, is:
A bob of heavy mass \(m\) is suspended by a light string of length \(l\). The bob is given a horizontal velocity \(v_0\) as shown in figure. If the string gets slack at some point P making an angle \( \theta \) from the horizontal, the ratio of the speed \(v\) of the bob at point P to its initial speed \(v_0\) is :
Moving charges generate an electric field and the rate of flow of charge is known as current. This is the basic concept in Electrostatics. Another important concept related to moving electric charges is the magnetic effect of current. Magnetism is caused by the current.
Region in space around a magnet where the Magnet has its Magnetic effect is called the Magnetic field of the Magnet. Let us suppose that there is a point charge q (moving with a velocity v and, located at r at a given time t) in presence of both the electric field E (r) and the magnetic field B (r). The force on an electric charge q due to both of them can be written as,
F = q [ E (r) + v × B (r)] ≡ EElectric +Fmagnetic
This force was based on the extensive experiments of Ampere and others. It is called the Lorentz force.