Note: In this question you may use without proof the result \( \dfrac{\d \ }{\d x}\big(\!\arctan x \big) = \dfrac 1 {1+x^2}\,\). Let \[ I_n = \int_0^1 x^n \arctan x \, \d x \;, \] where \(n=0\), 1, 2, 3, \(\ldots\) .
Solution:
The sequence of numbers \(x_0\), \(x_1\), \(x_2\), \(\ldots\) satisfies \[ x_{n+1} = \frac{ax_n-1}{x_n+b} \,. \] (You may assume that \(a\), \(b\) and \(x_0\) are such that \(x_n+b\ne0\,\).) Find an expression for \(x_{n+2}\) in terms of \(a\), \(b\) and \(x_n\).
Solution: \begin{align*} x_{n+2} &= \frac{ax_{n+1}-1}{x_{n+1}+b} \\ &= \frac{a \frac{ax_n - 1}{x_n+b}-1}{\frac{ax_n - 1}{x_n+b}+b} \\ &= \frac{a(ax_n-1)-(x_n+b)}{ax_n-1+b(x_n+b)} \\ &= \frac{(a^2-1)x_n-(a+b)}{(a+b)x_n+b^2-1} \end{align*}
Solution:
The Schwarz inequality is \[ \left( \int_a^b \f(x)\, \g(x)\,\d x\right)^{\!\!2} \le \left( \int_a^b \big( \f(x)\big)^2 \d x \right) \left( \int_a^b \big( \g(x)\big)^2 \d x \right) . \tag{\(*\)} \]
Solution:
A curve \(C\) is determined by the parametric equations \[ x=at^2 \, , \; y = 2at\,, \] where \(a > 0\).
Solution:
Let \[ S_n = \sum_{r=1}^n \frac 1 {\sqrt r \ } \,, \] where \(n\) is a positive integer.
Solution:
The functions \(\f\) and \(\g\) are defined, for \(x>0\), by \[ \f(x) = x^x\,, \ \ \ \ \ \g(x) = x^{\f(x)}\,. \]
Solution:
All vectors in this question lie in the same plane. The vertices of the non-right-angled triangle \(ABC\) have position vectors \(\bf a\), \(\bf b\) and \(\bf c\), respectively. The non-zero vectors \(\bf u\) and \(\bf v\) are perpendicular to \(BC\) and \(CA\), respectively. Write down the vector equation of the line through \(A\) perpendicular to \(BC\), in terms of \(\bf u\), \(\bf a\) and a parameter \(\lambda \). The line through \(A\) perpendicular to \(BC\) intersects the line through \(B\) perpendicular to \(CA\) at \(P\). Find the position vector of \(P\) in terms of \(\bf a\), \(\bf b\), \(\bf c\) and \(\bf u\). Hence show that the line \(CP\) is perpendicular to the line \(AB\).
Two identical rough cylinders of radius \(r\) and weight \(W\) rest, not touching each other but a negligible distance apart, on a horizontal floor. A thin flat rough plank of width \(2a\), where \(a < r\), and weight \(kW\) rests symmetrically and horizontally on the cylinders, with its length parallel to the axes of the cylinders and its faces horizontal. A vertical cross-section is shown in the diagram below. \vspace{1.1cm} \hspace{5.0cm} \begin{pspicture}(9.3,-5.00 ) \psset{xunit=1.0cm,yunit=1.0cm,algebraic=true,dotstyle=o,dotsize=3pt 0,linewidth=0.8pt,arrowsize=3pt 2,arrowinset=0.25} \psline(-2,-3)(7,-3) \pscircle(1,-1.5){1.50} \pscircle(4.02,-1.5 ){1.50} \psline[linewidth=3pt](1.45,-0.06)(3.58,-0.06) \end{pspicture} \vspace{-1.5cm} The coefficient of friction at all four contacts is \(\frac12\). The system is in equilibrium.
A car of mass \(m\) makes a journey of distance \(2d\) in a straight line. It experiences air resistance and rolling resistance so that the total resistance to motion when it is moving with speed \(v\) is \(Av^2 +R\), where \(A\) and \(R\) are constants. The car starts from rest and moves with constant acceleration \(a\) for a distance \(d\). Show that the work done by the engine for this half of the journey is \[ \int_0^d (ma+R+Av^2) \, \d x \] and that it can be written in the form \[ \int_0^w \frac {(ma+R+Av^2)v}a\; \d v \,, \] where \(w =\sqrt {2ad\,}\,\). For the second half of the journey, the acceleration of the car is \(-a\).