The momentum of the tackler and the halfback is the same before and after the tackle. There is no external force if you consider the tackler and the halfback as a system.
The total momentum before the tackle is \(\left( {{m_1}{v_1} + {m_2}{v_2}} \right)\).
And the total momentum after the tackle is \(\left( {{m_1} + {m_2}} \right)v\).
Using the concept of momentum conservation, you get
\(\begin{array}{c}\left( {{m_1} + {m_2}} \right)v = \left( {{m_1}{v_1} + {m_2}{v_2}} \right)\\v = \frac{{{m_1}{v_1} + {m_2}{v_2}}}{{{m_1} + {m_2}}}\\v = \frac{{\left[ {\left( {110\;{\rm{kg}}} \right) \times \left( { - 2.5\;{\rm{m/s}}} \right)} \right] + \left[ {\left( {82\;{\rm{kg}}} \right) \times \left( {5.0\;{\rm{m/s}}} \right)} \right]}}{{\left( {110\;{\rm{kg}}} \right) + \left( {82\;{\rm{kg}}} \right)}}\\v = 0.70\;{\rm{m/s}}{\rm{.}}\end{array}\)
Hence, their mutual speed is \(0.70\;{\rm{m/s}}\) immediately after the collision.