Let's start out by determining the force of weight, force normal and force parallel down the slope:
F_w= 50kg *9.8m/s^2= 490 NFw=50kg⋅9.8ms2=490N
F_n= 50kg*9.8m/s^2*cos(10^@)=482.6 NFn=50kg⋅9.8ms2⋅cos(10∘)=482.6N
F_p= 50 kg*9.8m/s^2*sin(10^@)=85.1 NFp=50kg⋅9.8ms2⋅sin(10∘)=85.1N
So we have the force parallel that want to pull the box down the ramp, so we know that the force of static friction must be at least equal to force parallel, to make the object not move:
F_n*u_s >= F_pFn⋅us≥Fp
u_s>=F_p/F_nus≥FpFn
u_s>="85.1 N"/"482.6 N"us≥85.1 N482.6 N
u_s>=0.176us≥0.176
Ok, so this girl is pushing down the box down the ramp, the force parallel will work in her favor, while the force of friction will not so:
F_F= F_n*u_kFF=Fn⋅uk
F_F= 482.6 N*0.19= 91.694 NFF=482.6N⋅0.19=91.694N
F_"net"= 50 N+85.1 N-91.694 N= 43.406 NFnet=50N+85.1N−91.694N=43.406N
The work energy conservation theorem states:
W= KE_f-KE_iW=KEf−KEi
The initial KE energy is 0 J as the box is not moving so:
(43.406 N)(5 m)= 1/2(50 kg)v^2(43.406N)(5m)=12(50kg)v2
v= 2.95 m/sv=2.95ms
The third part I'm not entirely sure of but, 20^@20∘ below the horizontal would still mean that the inclination of the ramp, from the bottom of the ramp at the other horizontal is 20^@20∘
a= F_"net"/ma=Fnetm
F_p= 50 kg*9.8m/s^2*sin(20^@)=167.59 NFp=50kg⋅9.8ms2⋅sin(20∘)=167.59N
F_n= 50 kg*9.8m/s^2*cos(20^@)=460.45 NFn=50kg⋅9.8ms2⋅cos(20∘)=460.45N
F_f= 460.45*0.19= 87.486 NFf=460.45⋅0.19=87.486N
F_"net"= 167.59 N-87.486 N= 80.104 NFnet=167.59N−87.486N=80.104N
a= "80.104 N"/"50 kg"a=80.104 N50 kg
a= 1.6 m/s^2a=1.6ms2