\(R = 8Ω\)
\(Φ=\frac{2}{3}(9−t^2)\)
At\( t = 3, φ = 0\)
\(∈ =|−\frac{dΦ}{dt}|=\frac{4}{3t}\)
\(H=∫_0^3\frac{V^2}{R}dt=∫_0^3\frac{1}{8}×16/9t^2dt\)
= \(\frac{2}{9} \times \bigg(\frac{t^3}{3}\bigg)^3_0 \)
= \(\frac{2}{9} \times 3 \times 27\)
= \(2\) \(J\)
A bob of mass \(m\) is suspended at a point \(O\) by a light string of length \(l\) and left to perform vertical motion (circular) as shown in the figure. Initially, by applying horizontal velocity \(v_0\) at the point ‘A’, the string becomes slack when the bob reaches at the point ‘D’. The ratio of the kinetic energy of the bob at the points B and C is:
Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is:
Resistance is the measure of opposition applied by any object to the flow of electric current. A resistor is an electronic constituent that is used in the circuit with the purpose of offering that specific amount of resistance.
R=V/I
In this case,
v = Voltage across its ends
I = Current flowing through it
All materials resist current flow to some degree. They fall into one of two broad categories:
Resistance measurements are normally taken to indicate the condition of a component or a circuit.