Early railways, roads, and roller coasters often connected straight track directly to circular arcs. The pieces matched in position and direction, so the connection looked smooth.
The hidden problem was curvature: at the instant the track switched from straight to circular, curvature jumped from \(0\) to \(1/R\). Since normal acceleration is \(a_N=\kappa v^2\), that jump becomes a sudden change in rider force.
Modern designs use transition curves such as a clothoid or Euler spiral. Along an Euler spiral, curvature changes gradually with distance, so the rider eases into the turn.