No, the top speed performance is not enough. To calculate any climb speed one needs to know at which flight speed this climb takes place. Per definition, the climb speed is zero at top speed.
Next, it helps to have some more information about the airframe. The wing's aspect ratio is an important factor because climb happens at lower speed when induced drag is a higher proportion of total drag.
So I need to make two more assumptions in order to find the climb speed:
- You want to know the maximum climb speed at sea level.
- I am allowed to use information from this answer to complete my knowledge.
Now for the climb speed calculation, which can already be found in several older answers: The flight speed for maximum climb rate is when induced drag is three times as large as zero-lift drag. The first step is to determine the correct polar point. This is a bit more tricky than it sounds because the zero-lift drag coefficient depends on the flight speed and air temperature. Let's start with 0.029 and see where that brings us to:
$$c_{L_{opt.\,climb}} = \sqrt{3\cdot c_{D0}\cdot\pi\cdot AR\cdot\epsilon} = \text{1.48}$$
That corresponds to a flight speed of
$$v_{opt.\,climb} = \sqrt{\frac{2\cdot m\cdot g}{c_{L_{opt.\,climb}}\cdot\rho\cdot S}} = \text{39.7 m/s}$$
calculated with the MTOW of the XB-42 of 15,060 kg. Now we can determine the ratio of the Reynolds numbers between climb and maximum speed which is 0.2915. If I assume that the zero-lift drag changes in proportion to $\left(\frac{1}{Re}\right)^{0.2}$, the zero-lift drag at best climb speed rises to 0.02907. Close enough.
However, this speed is rather close to what I suspect is the stall speed of a clean XB-42, and extending flaps will create more drag. Therefore, it will be better to climb at a higher speed, say 50 m/s, and see how fast it climbs there. The zero-lift drag at that speed is scaled to 0.0276 and the lift coefficient to 0.933. Now to the climb speed:
$$v_z = \frac{P_{mot}\cdot\eta_P}{m\cdot g} - \frac{\frac{\rho\cdot v^3}{2}\cdot S\cdot\left(c_{D0}+\frac{c_L^2}{\pi\cdot AR\cdot\epsilon}\right)}{m\cdot g} = \text{12.57 m/s}$$
The symbols used are:
$\kern{5mm} \rho\:\:\:\:\:$ air density = 1.225 kg/m³ at sea level
$\kern{5mm} v\:\:\:\:\:$ flight speed
$\kern{5mm} S\:\:\:\:\:$ wing surface area = 51.6 m²
$\kern{5mm} c_{D0} \:$ zero-lift drag coefficient at 183.3 m/s and 7140 m
$\kern{5mm} c_L \:\:\:$ lift coefficient
$\kern{5mm} \pi \:\:\:\:\:$ 3.14159$\dots$
$\kern{5mm} AR \:\:$ aspect ratio of the wing = 8.95
$\kern{5mm} \epsilon \:\:\:\:\:\:$ the wing's Oswald factor = 0.9
$\kern{5mm} m \:\:\:\;$ aircraft mass = 15,080 kg
$\kern{5mm} g \:\:\:\:\;$ gravitational acceleration
$\kern{5mm} P \:\:\:\:\:$ engine shaft power = 2498 kW
$\kern{5mm} \eta_P \:\:\;$ propeller efficiency = 0.85