As the board is raised by an angle <em>θ</em>, the block will be held in place by 3 forces:
• its weight, pointing downward (magnitude <em>w</em> )
• the normal force of the board pushing up on the block, pointing in the direction perpendicular to the board (mag. <em>n</em>)
• static friction, pointing in the direction parallel to the board, opposite the direction the block would slip (mag. <em>f</em> )
Decompose the vectors into components that are parallel and perpendicular to the board (taking the direction of <em>n</em> to be the positive direction perpendicular to the board, and the direction of <em>f</em> to be the negative directoin parallel to it), so that by Newton's second law, we have
• net parallel force:
∑ <em>F</em> = <em>w</em> (//) + <em>f</em>
∑ <em>F</em> = <em>m g </em>sin(<em>θ</em>) - <em>µ</em> <em>n</em> = 0
where <em>µ</em> = 0.45 is the coefficient of static friction, <em>g</em> = 9.80 m/s² is the mag. of the acceleration due to gravity, and <em>m</em> = 15.0 kg is the mass of the block.
• net perpendicular force:
∑ <em>F</em> = <em> n</em> + <em>w</em> (⟂)
∑ <em>F</em> = <em>n</em> - <em>m g</em> cos(<em>θ</em>) = 0
Solve for <em>n</em> in the equation for net perpendicular force:
<em>n</em> = <em>m g</em> cos(<em>θ</em>)
Substitute this into the equation for net parallel force:
<em>m g </em>sin(<em>θ</em>) - 0.45 <em>m g</em> cos(<em>θ</em>) = 0
Solve for <em>θ</em> :
sin(<em>θ</em>) - 0.45 cos(<em>θ</em>) = 0
sin(<em>θ</em>) = 0.45 cos(<em>θ</em>)
tan(<em>θ</em>) = 0.45
<em>θ</em> = tan⁻¹(0.45)
<em>θ</em> ≈ 24.2°
So the maximum angle the board can be lifted before the block starts to slide is about 24.2°, since the coefficient of static friction <em>µ</em> is such that
<em>f</em> = <em>µ</em> <em>n</em>
where <em>f</em> is the maximum magnitude of the static friction force.