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A block of mass $m$ is pushed by a force of magnitude $F$, which acts at an angle of $\theta$ to the horizontal, as shown above.

The magnitude of the normal force between the block and the surface is

A

$mg$

B

$mg+F\cos\theta$

C

$mg-F\cos\theta$

D

$mg-F\sin\theta$

E

$mg+F\sin\theta$

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